{"facets":[{"max_values":5,"printable_name":"Observables","type":"observables","vals":[{"doc_count":2231,"key":"SIG","url_params":{"observables":"SIG"}},{"doc_count":324,"key":"DSIG/DT","url_params":{"observables":"DSIG/DT"}},{"doc_count":298,"key":"MULT","url_params":{"observables":"MULT"}},{"doc_count":250,"key":"N","url_params":{"observables":"N"}},{"doc_count":244,"key":"POL","url_params":{"observables":"POL"}},{"doc_count":227,"key":"SLOPE","url_params":{"observables":"SLOPE"}},{"doc_count":216,"key":"ASYM","url_params":{"observables":"ASYM"}},{"doc_count":216,"key":"DSIG/DX","url_params":{"observables":"DSIG/DX"}},{"doc_count":211,"key":"DSIG/DOMEGA","url_params":{"observables":"DSIG/DOMEGA"}},{"doc_count":205,"key":"DSIG/DPT","url_params":{"observables":"DSIG/DPT"}}]},{"max_values":5,"printable_name":"Subject_areas","type":"subject_areas","vals":[{"doc_count":4579,"key":"hep-ex","url_params":{"subject_areas":"hep-ex"}},{"doc_count":1260,"key":"nucl-ex","url_params":{"subject_areas":"nucl-ex"}},{"doc_count":68,"key":"Phenomenology-HEP","url_params":{"subject_areas":"Phenomenology-HEP"}},{"doc_count":55,"key":"nucl-th","url_params":{"subject_areas":"nucl-th"}},{"doc_count":54,"key":"hep-ph","url_params":{"subject_areas":"hep-ph"}},{"doc_count":14,"key":"Instrumentation","url_params":{"subject_areas":"Instrumentation"}},{"doc_count":11,"key":"Astrophysics","url_params":{"subject_areas":"Astrophysics"}},{"doc_count":11,"key":"physics.ins-det","url_params":{"subject_areas":"physics.ins-det"}},{"doc_count":5,"key":"astro-ph.CO","url_params":{"subject_areas":"astro-ph.CO"}},{"doc_count":3,"key":"Accelerators","url_params":{"subject_areas":"Accelerators"}}]},{"max_values":5,"printable_name":"Collaboration","type":"collaboration","vals":[{"doc_count":604,"key":"CMS","url_params":{"collaboration":"CMS"}},{"doc_count":336,"key":"ATLAS","url_params":{"collaboration":"ATLAS"}},{"doc_count":241,"key":"STAR","url_params":{"collaboration":"STAR"}},{"doc_count":211,"key":"PHENIX","url_params":{"collaboration":"PHENIX"}},{"doc_count":201,"key":"CDF","url_params":{"collaboration":"CDF"}},{"doc_count":170,"key":"ZEUS","url_params":{"collaboration":"ZEUS"}},{"doc_count":149,"key":"H1","url_params":{"collaboration":"H1"}},{"doc_count":144,"key":"OPAL","url_params":{"collaboration":"OPAL"}},{"doc_count":126,"key":"D0","url_params":{"collaboration":"D0"}},{"doc_count":112,"key":"L3","url_params":{"collaboration":"L3"}}]},{"max_values":10,"printable_name":"Authors","type":"author","vals":[{"doc_count":1139,"key":"Sharma, Archana","url_params":{"author":"Sharma, Archana"}},{"doc_count":912,"key":"M\u00fcller, Thomas","url_params":{"author":"M\u00fcller, Thomas"}},{"doc_count":864,"key":"Ahmad, Muhammad","url_params":{"author":"Ahmad, Muhammad"}},{"doc_count":781,"key":"Bocci, Andrea","url_params":{"author":"Bocci, Andrea"}},{"doc_count":713,"key":"Eckerlin, Guenter","url_params":{"author":"Eckerlin, Guenter"}},{"doc_count":711,"key":"Lebedev, A.","url_params":{"author":"Lebedev, A."}},{"doc_count":702,"key":"Geralis, Theodoros","url_params":{"author":"Geralis, Theodoros"}},{"doc_count":679,"key":"Bagliesi, Giuseppe","url_params":{"author":"Bagliesi, Giuseppe"}},{"doc_count":678,"key":"Rolandi, Gigi","url_params":{"author":"Rolandi, Gigi"}},{"doc_count":664,"key":"Van Doninck, Walter","url_params":{"author":"Van Doninck, Walter"}}]},{"max_values":5,"printable_name":"Reactions","type":"reactions","vals":[{"doc_count":217,"key":"E+ E- --> HADRONS","url_params":{"reactions":"E+ E- --> HADRONS"}},{"doc_count":118,"key":"E+ E- --> Z0","url_params":{"reactions":"E+ E- --> Z0"}},{"doc_count":110,"key":"P P --> P P","url_params":{"reactions":"P P --> P P"}},{"doc_count":68,"key":"PI- P --> PI- P","url_params":{"reactions":"PI- P --> PI- P"}},{"doc_count":64,"key":"PBAR P --> PBAR P","url_params":{"reactions":"PBAR P --> PBAR P"}},{"doc_count":54,"key":"E+ E- --> CHARGED X","url_params":{"reactions":"E+ E- --> CHARGED X"}},{"doc_count":54,"key":"E+ E- --> MU+ MU-","url_params":{"reactions":"E+ E- --> MU+ MU-"}},{"doc_count":54,"key":"P P --> X","url_params":{"reactions":"P P --> X"}},{"doc_count":54,"key":"PI+ P --> PI+ P","url_params":{"reactions":"PI+ P --> PI+ P"}},{"doc_count":50,"key":"P P --> TOP TOPBAR X","url_params":{"reactions":"P P --> TOP TOPBAR X"}}]},{"max_values":5,"printable_name":"Date","type":"date","vals":[{"doc_count":197,"key":2023,"key_as_string":"2023-01-01T00:00:00.000Z","url_params":{"date":2023}},{"doc_count":168,"key":2016,"key_as_string":"2016-01-01T00:00:00.000Z","url_params":{"date":2016}},{"doc_count":153,"key":1997,"key_as_string":"1997-01-01T00:00:00.000Z","url_params":{"date":1997}},{"doc_count":152,"key":1995,"key_as_string":"1995-01-01T00:00:00.000Z","url_params":{"date":1995}},{"doc_count":150,"key":2018,"key_as_string":"2018-01-01T00:00:00.000Z","url_params":{"date":2018}},{"doc_count":148,"key":2000,"key_as_string":"2000-01-01T00:00:00.000Z","url_params":{"date":2000}},{"doc_count":145,"key":1996,"key_as_string":"1996-01-01T00:00:00.000Z","url_params":{"date":1996}},{"doc_count":143,"key":2017,"key_as_string":"2017-01-01T00:00:00.000Z","url_params":{"date":2017}},{"doc_count":132,"key":1990,"key_as_string":"1990-01-01T00:00:00.000Z","url_params":{"date":1990}},{"doc_count":128,"key":2001,"key_as_string":"2001-01-01T00:00:00.000Z","url_params":{"date":2001}},{"doc_count":126,"key":1998,"key_as_string":"1998-01-01T00:00:00.000Z","url_params":{"date":1998}},{"doc_count":123,"key":1999,"key_as_string":"1999-01-01T00:00:00.000Z","url_params":{"date":1999}},{"doc_count":121,"key":2022,"key_as_string":"2022-01-01T00:00:00.000Z","url_params":{"date":2022}},{"doc_count":119,"key":2007,"key_as_string":"2007-01-01T00:00:00.000Z","url_params":{"date":2007}},{"doc_count":118,"key":1991,"key_as_string":"1991-01-01T00:00:00.000Z","url_params":{"date":1991}},{"doc_count":116,"key":1984,"key_as_string":"1984-01-01T00:00:00.000Z","url_params":{"date":1984}},{"doc_count":113,"key":1988,"key_as_string":"1988-01-01T00:00:00.000Z","url_params":{"date":1988}},{"doc_count":112,"key":1983,"key_as_string":"1983-01-01T00:00:00.000Z","url_params":{"date":1983}},{"doc_count":111,"key":2015,"key_as_string":"2015-01-01T00:00:00.000Z","url_params":{"date":2015}},{"doc_count":108,"key":2021,"key_as_string":"2021-01-01T00:00:00.000Z","url_params":{"date":2021}},{"doc_count":108,"key":2014,"key_as_string":"2014-01-01T00:00:00.000Z","url_params":{"date":2014}},{"doc_count":107,"key":1985,"key_as_string":"1985-01-01T00:00:00.000Z","url_params":{"date":1985}},{"doc_count":105,"key":1982,"key_as_string":"1982-01-01T00:00:00.000Z","url_params":{"date":1982}},{"doc_count":103,"key":1989,"key_as_string":"1989-01-01T00:00:00.000Z","url_params":{"date":1989}},{"doc_count":100,"key":2010,"key_as_string":"2010-01-01T00:00:00.000Z","url_params":{"date":2010}},{"doc_count":100,"key":1987,"key_as_string":"1987-01-01T00:00:00.000Z","url_params":{"date":1987}},{"doc_count":99,"key":1981,"key_as_string":"1981-01-01T00:00:00.000Z","url_params":{"date":1981}},{"doc_count":98,"key":1994,"key_as_string":"1994-01-01T00:00:00.000Z","url_params":{"date":1994}},{"doc_count":97,"key":2009,"key_as_string":"2009-01-01T00:00:00.000Z","url_params":{"date":2009}},{"doc_count":94,"key":1980,"key_as_string":"1980-01-01T00:00:00.000Z","url_params":{"date":1980}},{"doc_count":93,"key":1993,"key_as_string":"1993-01-01T00:00:00.000Z","url_params":{"date":1993}},{"doc_count":92,"key":1992,"key_as_string":"1992-01-01T00:00:00.000Z","url_params":{"date":1992}},{"doc_count":92,"key":1986,"key_as_string":"1986-01-01T00:00:00.000Z","url_params":{"date":1986}},{"doc_count":90,"key":1978,"key_as_string":"1978-01-01T00:00:00.000Z","url_params":{"date":1978}},{"doc_count":89,"key":2013,"key_as_string":"2013-01-01T00:00:00.000Z","url_params":{"date":2013}},{"doc_count":88,"key":1976,"key_as_string":"1976-01-01T00:00:00.000Z","url_params":{"date":1976}},{"doc_count":86,"key":2020,"key_as_string":"2020-01-01T00:00:00.000Z","url_params":{"date":2020}},{"doc_count":86,"key":2011,"key_as_string":"2011-01-01T00:00:00.000Z","url_params":{"date":2011}},{"doc_count":84,"key":2019,"key_as_string":"2019-01-01T00:00:00.000Z","url_params":{"date":2019}},{"doc_count":82,"key":2008,"key_as_string":"2008-01-01T00:00:00.000Z","url_params":{"date":2008}},{"doc_count":82,"key":2004,"key_as_string":"2004-01-01T00:00:00.000Z","url_params":{"date":2004}},{"doc_count":80,"key":2012,"key_as_string":"2012-01-01T00:00:00.000Z","url_params":{"date":2012}},{"doc_count":80,"key":2006,"key_as_string":"2006-01-01T00:00:00.000Z","url_params":{"date":2006}},{"doc_count":80,"key":1979,"key_as_string":"1979-01-01T00:00:00.000Z","url_params":{"date":1979}},{"doc_count":78,"key":2005,"key_as_string":"2005-01-01T00:00:00.000Z","url_params":{"date":2005}},{"doc_count":78,"key":2003,"key_as_string":"2003-01-01T00:00:00.000Z","url_params":{"date":2003}},{"doc_count":76,"key":1977,"key_as_string":"1977-01-01T00:00:00.000Z","url_params":{"date":1977}},{"doc_count":72,"key":2002,"key_as_string":"2002-01-01T00:00:00.000Z","url_params":{"date":2002}},{"doc_count":68,"key":1975,"key_as_string":"1975-01-01T00:00:00.000Z","url_params":{"date":1975}},{"doc_count":52,"key":1973,"key_as_string":"1973-01-01T00:00:00.000Z","url_params":{"date":1973}},{"doc_count":36,"key":1974,"key_as_string":"1974-01-01T00:00:00.000Z","url_params":{"date":1974}},{"doc_count":35,"key":1972,"key_as_string":"1972-01-01T00:00:00.000Z","url_params":{"date":1972}},{"doc_count":34,"key":1971,"key_as_string":"1971-01-01T00:00:00.000Z","url_params":{"date":1971}},{"doc_count":23,"key":2024,"key_as_string":"2024-01-01T00:00:00.000Z","url_params":{"date":2024}},{"doc_count":18,"key":1970,"key_as_string":"1970-01-01T00:00:00.000Z","url_params":{"date":1970}},{"doc_count":16,"key":1968,"key_as_string":"1968-01-01T00:00:00.000Z","url_params":{"date":1968}},{"doc_count":12,"key":1969,"key_as_string":"1969-01-01T00:00:00.000Z","url_params":{"date":1969}},{"doc_count":12,"key":1966,"key_as_string":"1966-01-01T00:00:00.000Z","url_params":{"date":1966}},{"doc_count":10,"key":1965,"key_as_string":"1965-01-01T00:00:00.000Z","url_params":{"date":1965}},{"doc_count":9,"key":1967,"key_as_string":"1967-01-01T00:00:00.000Z","url_params":{"date":1967}},{"doc_count":5,"key":1964,"key_as_string":"1964-01-01T00:00:00.000Z","url_params":{"date":1964}},{"doc_count":4,"key":1961,"key_as_string":"1961-01-01T00:00:00.000Z","url_params":{"date":1961}},{"doc_count":3,"key":1963,"key_as_string":"1963-01-01T00:00:00.000Z","url_params":{"date":1963}},{"doc_count":3,"key":1962,"key_as_string":"1962-01-01T00:00:00.000Z","url_params":{"date":1962}},{"doc_count":1,"key":1960,"key_as_string":"1960-01-01T00:00:00.000Z","url_params":{"date":1960}},{"doc_count":1,"key":1956,"key_as_string":"1956-01-01T00:00:00.000Z","url_params":{"date":1956}},{"doc_count":0,"key":1959,"key_as_string":"1959-01-01T00:00:00.000Z","url_params":{"date":1959}},{"doc_count":0,"key":1958,"key_as_string":"1958-01-01T00:00:00.000Z","url_params":{"date":1958}},{"doc_count":0,"key":1957,"key_as_string":"1957-01-01T00:00:00.000Z","url_params":{"date":1957}}]},{"max_values":5,"printable_name":"Phrases","type":"phrases","vals":[{"doc_count":2416,"key":"Inclusive","url_params":{"phrases":"Inclusive"}},{"doc_count":2281,"key":"Cross Section","url_params":{"phrases":"Cross Section"}},{"doc_count":2192,"key":"Integrated Cross Section","url_params":{"phrases":"Integrated Cross Section"}},{"doc_count":1972,"key":"Exclusive","url_params":{"phrases":"Exclusive"}},{"doc_count":1341,"key":"Single Differential Cross Section","url_params":{"phrases":"Single Differential Cross Section"}},{"doc_count":936,"key":"E+ E- Scattering","url_params":{"phrases":"E+ E- Scattering"}},{"doc_count":879,"key":"Proton-Proton Scattering","url_params":{"phrases":"Proton-Proton Scattering"}},{"doc_count":861,"key":"Electron production","url_params":{"phrases":"Electron production"}},{"doc_count":802,"key":"Strange production","url_params":{"phrases":"Strange production"}},{"doc_count":599,"key":"Muon production","url_params":{"phrases":"Muon production"}}]},{"max_values":5,"printable_name":"CM Energies (GeV)","type":"cmenergies","vals":[{"doc_count":null,"key":"0.0 \u2264 \u221as < 1.0","url_params":{"cmenergies":"0.0,1.0"}},{"doc_count":null,"key":"1.0 \u2264 \u221as < 2.0","url_params":{"cmenergies":"1.0,2.0"}},{"doc_count":null,"key":"2.0 \u2264 \u221as < 5.0","url_params":{"cmenergies":"2.0,5.0"}},{"doc_count":null,"key":"5.0 \u2264 \u221as < 10.0","url_params":{"cmenergies":"5.0,10.0"}},{"doc_count":null,"key":"10.0 \u2264 \u221as < 100.0","url_params":{"cmenergies":"10.0,100.0"}},{"doc_count":null,"key":"100.0 \u2264 \u221as < 1000.0","url_params":{"cmenergies":"100.0,1000.0"}},{"doc_count":null,"key":"1000.0 \u2264 \u221as < 7000.0","url_params":{"cmenergies":"1000.0,7000.0"}},{"doc_count":null,"key":"7000.0 \u2264 \u221as < 8000.0","url_params":{"cmenergies":"7000.0,8000.0"}},{"doc_count":null,"key":"8000.0 \u2264 \u221as < 13000.0","url_params":{"cmenergies":"8000.0,13000.0"}},{"doc_count":null,"key":"\u221as \u2265 13000.0","url_params":{"cmenergies":"13000.0,100000.0"}}]}],"hits":{"total":5544},"results":[{"abstract":"A search for a new $Z'$ gauge boson predicted by $L_{\\mu}-L_{\\tau}$ models, based on charged-current Drell-Yan production, $pp \\rightarrow W^{\\pm(*)} \\rightarrow Z' \\mu^{\\pm} \\nu \\rightarrow \\mu^{\\pm}\\mu^{\\mp}\\mu^{\\pm}\\nu$, is presented. The data sample used corresponds to an integrated luminosity of 140 fb$^{-1}$ of proton-proton collisions at $\\sqrt{s} = 13$ TeV recorded by the ATLAS detector at the Large Hadron Collider. The search examines a final state of $3\\mu$ plus large missing transverse momentum. Upper limits are set on the $Z'$ production cross-section times branching ratio in the mass range of 5-81 GeV. After combining with the previous $Z'$ search using the neutral-current Drell-Yan production with a $4\\mu$ final state, the most stringent exclusion limits to date are achieved in the parameter space of the $Z'$ coupling strength and mass.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2761384/1/csv","json":"https://www.hepdata.net/download/submission/ins2761384/1/json","root":"https://www.hepdata.net/download/submission/ins2761384/1/root","yaml":"https://www.hepdata.net/download/submission/ins2761384/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2761384/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2402.15212","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming"],"collaborations":["ATLAS"],"control_number":"149991","creation_date":"2024-02-23","data":[{"abstract":"Observed and expected upper limits at 95% CL on the production cross-section times branching fraction of the process $pp\\to W\\to Z^{\\prime}$ $\\mu \\nu \\to \\mu \\mu \\mu \\nu$ as a function of $m_{Z^{\\prime}}$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2761384/Upper limits on production cross-section times BR/csv","json":"https://www.hepdata.net/download/table/ins2761384/Upper limits on production cross-section times BR/json","root":"https://www.hepdata.net/download/table/ins2761384/Upper limits on production cross-section times BR/root","yaml":"https://www.hepdata.net/download/table/ins2761384/Upper limits on production cross-section times BR/yaml","yoda":"https://www.hepdata.net/download/table/ins2761384/Upper limits on production cross-section times BR/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150530","creation_date":"2024-02-23","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["Upper limits"]},"date":"23 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149991.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150530,"inspire_id":"2761384","journal_info":"CERN-EP-2024-042","keywords":[{"name":"observables","synonyms":"","value":"Upper limits"},{"name":"cmenergies","synonyms":"","value":"13000"}],"last_updated":"2024-03-26T08:44:52","parent_child_join":{"name":"child_datatable","parent":"149991"},"recid":150530,"related_publication":149991,"title":"Upper limits on production cross-section times BR","uuid":"14f496cd-83e0-466d-99ea-48547d07b3b9"},{"abstract":"Observed and expected upper limits at 95% CL on the coupling parameter $g_{Z^{\\prime}}$ as a function of $m_{Z^{\\prime}}$ from the statistical combination of the $3\\mu$ and $4\\mu$ channels.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2761384/Upper limits on the coupling parameter $g_{Z^{%5Cprime}}$/csv","json":"https://www.hepdata.net/download/table/ins2761384/Upper limits on the coupling parameter $g_{Z^{%5Cprime}}$/json","root":"https://www.hepdata.net/download/table/ins2761384/Upper limits on the coupling parameter $g_{Z^{%5Cprime}}$/root","yaml":"https://www.hepdata.net/download/table/ins2761384/Upper limits on the coupling parameter $g_{Z^{%5Cprime}}$/yaml","yoda":"https://www.hepdata.net/download/table/ins2761384/Upper limits on the coupling parameter $g_{Z^{%5Cprime}}$/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150531","creation_date":"2024-02-23","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["Upper limits"]},"date":"23 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149991.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150531,"inspire_id":"2761384","journal_info":"CERN-EP-2024-042","keywords":[{"name":"observables","synonyms":"","value":"Upper limits"},{"name":"cmenergies","synonyms":"","value":"13000"}],"last_updated":"2024-03-26T08:44:52","parent_child_join":{"name":"child_datatable","parent":"149991"},"recid":150531,"related_publication":149991,"title":"Upper limits on the coupling parameter $g_{Z^{\\prime}}$","uuid":"0935a8de-3b55-4eb4-9b0e-49f3a7c6f4e7"},{"abstract":"Exclusion contour compared to the limits from the Neutrino Trident and the $B_{S}$ mixing experimental results.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2761384/Exclusion contour/csv","json":"https://www.hepdata.net/download/table/ins2761384/Exclusion contour/json","root":"https://www.hepdata.net/download/table/ins2761384/Exclusion contour/root","yaml":"https://www.hepdata.net/download/table/ins2761384/Exclusion contour/yaml","yoda":"https://www.hepdata.net/download/table/ins2761384/Exclusion contour/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150532","creation_date":"2024-02-23","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["Upper limits"]},"date":"23 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149991.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150532,"inspire_id":"2761384","journal_info":"CERN-EP-2024-042","keywords":[{"name":"observables","synonyms":"","value":"Upper limits"},{"name":"cmenergies","synonyms":"","value":"13000"}],"last_updated":"2024-03-26T08:44:52","parent_child_join":{"name":"child_datatable","parent":"149991"},"recid":150532,"related_publication":149991,"title":"Exclusion contour","uuid":"352f8177-08c0-432b-9661-139b264a4915"},{"abstract":"Summary of observed and expected background yields in the SR after the likelihood fit under the background-only hypothesis.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2761384/Yields in the SR/csv","json":"https://www.hepdata.net/download/table/ins2761384/Yields in the SR/json","root":"https://www.hepdata.net/download/table/ins2761384/Yields in the SR/root","yaml":"https://www.hepdata.net/download/table/ins2761384/Yields in the SR/yaml","yoda":"https://www.hepdata.net/download/table/ins2761384/Yields in the SR/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150533","creation_date":"2024-02-23","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["Yields"]},"date":"23 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149991.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150533,"inspire_id":"2761384","journal_info":"CERN-EP-2024-042","keywords":[{"name":"observables","synonyms":"","value":"Yields"},{"name":"cmenergies","synonyms":"","value":"13000"}],"last_updated":"2024-03-26T08:44:52","parent_child_join":{"name":"child_datatable","parent":"149991"},"recid":150533,"related_publication":149991,"title":"Yields in the SR","uuid":"4334c63f-d2b2-476d-8e14-a6b3041fb528"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["Upper limits","Yields"]},"date":"23 Feb 2024","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.149991","id":149991,"inspire_id":"2761384","journal_info":"CERN-EP-2024-042","keywords":[{"schema":"INSPIRE","source":"classifier","value":"p p, scattering"},{"schema":"INSPIRE","source":"classifier","value":"transverse momentum, missing-energy"},{"schema":"INSPIRE","source":"classifier","value":"Drell-Yan process"},{"schema":"INSPIRE","source":"classifier","value":"gauge boson"},{"schema":"INSPIRE","source":"classifier","value":"ATLAS"},{"schema":"INSPIRE","source":"classifier","value":"TeV"},{"schema":"INSPIRE","source":"classifier","value":"GeV"},{"schema":"INSPIRE","source":"classifier","value":"branching ratio"},{"schema":"INSPIRE","source":"classifier","value":"charged current"},{"schema":"INSPIRE","source":"classifier","value":"CERN LHC Coll"},{"schema":"INSPIRE","source":"classifier","value":"coupling constant"},{"schema":"INSPIRE","source":"classifier","value":"neutral current"}],"last_updated":"2024-03-26T08:44:53","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-03-26T00:00:00","recid":149991,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"}],"title":"Search for a new $Z'$ gauge boson via the $pp \\rightarrow W^{\\pm(*)} \\rightarrow Z' \\mu^{\\pm} \\nu \\rightarrow \\mu^{\\pm}\\mu^{\\mp}\\mu^{\\pm}\\nu$ process in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","total_tables":4,"type":["article"],"uuid":"2204245e-3d33-479d-a38e-38d38a961f11","version":1,"year":"2024"},{"abstract":"Statistical combinations of searches for charginos and neutralinos using various decay channels are performed using $139\\,$fb$^{-1}$ of $pp$ collision data at $\\sqrt{s}=13\\,$TeV with the ATLAS detector at the Large Hadron Collider. Searches targeting pure-wino chargino pair production, pure-wino chargino-neutralino production, or higgsino production decaying via Standard Model $W$, $Z$, or $h$ bosons are combined to extend the mass reach to the produced SUSY particles by 30-100 GeV. The depth of the sensitivity of the original searches is also improved by the combinations, lowering the 95% CL cross-section upper limits by 15%-40%.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2758009/1/csv","json":"https://www.hepdata.net/download/submission/ins2758009/1/json","root":"https://www.hepdata.net/download/submission/ins2758009/1/root","yaml":"https://www.hepdata.net/download/submission/ins2758009/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2758009/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2402.08347","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"149530","creation_date":"2024-02-13","data":[{"abstract":"Expected 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 1/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150044","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150044,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150044,"related_publication":149530,"title":"Table 1","uuid":"5a1236dd-ecea-46ab-874a-168fed939bbb"},{"abstract":"$+1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 2/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150045","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150045,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150045,"related_publication":149530,"title":"Table 2","uuid":"9f57f08d-b836-48fe-86ef-ad9ac55b781e"},{"abstract":"$-1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 3/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 3/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150046","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150046,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150046,"related_publication":149530,"title":"Table 3","uuid":"f30b878f-f665-40ac-b2a1-08e8ecc7cb79"},{"abstract":"Observed 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 4/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 4/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 4/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150047","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150047,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150047,"related_publication":149530,"title":"Table 4","uuid":"e38c4dea-d27c-4838-9a84-fc5818600221"},{"abstract":"$+1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 5/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 5/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 5/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150048","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150048,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150048,"related_publication":149530,"title":"Table 5","uuid":"e539b944-6e5c-4dad-8a1f-d6dbe2d0c41b"},{"abstract":"$-1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 6/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 6/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 6/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 6/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 6/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150049","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150049,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150049,"related_publication":149530,"title":"Table 6","uuid":"7edd7c9a-c2f1-46b0-8642-44ba022e8bb8"},{"abstract":"Expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 7/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 7/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 7/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 7/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 7/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150050","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150050,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150050,"related_publication":149530,"title":"Table 7","uuid":"eb2d8af8-729d-491a-b451-e74a3e15c670"},{"abstract":"$+1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 8/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 8/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 8/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 8/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 8/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150051","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150051,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150051,"related_publication":149530,"title":"Table 8","uuid":"9d97a0c9-bdaf-4119-b462-2bc01cc68007"},{"abstract":"$-1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 9/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 9/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 9/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 9/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 9/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150052","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150052,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150052,"related_publication":149530,"title":"Table 9","uuid":"81913b40-074a-49fa-b595-ee2d2f1ff3f6"},{"abstract":"Observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 10/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 10/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 10/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 10/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 10/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150053","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150053,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150053,"related_publication":149530,"title":"Table 10","uuid":"5a282597-ce94-4d60-a7e0-98410cf7213f"},{"abstract":"$+1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 11/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 11/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 11/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 11/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 11/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150054","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150054,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150054,"related_publication":149530,"title":"Table 11","uuid":"dea67f6c-57a1-45c1-8860-20dd5e1d0959"},{"abstract":"$-1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 12/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 12/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 12/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 12/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 12/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150055","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150055,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150055,"related_publication":149530,"title":"Table 12","uuid":"14c0c879-7c5a-4d78-bc31-86be789a83d5"},{"abstract":"Expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 13/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 13/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 13/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 13/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 13/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150056","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150056,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150056,"related_publication":149530,"title":"Table 13","uuid":"54e31da5-1da6-4745-a299-eaeab64e0903"},{"abstract":"$+1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 14/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 14/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 14/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 14/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 14/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150057","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150057,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150057,"related_publication":149530,"title":"Table 14","uuid":"7c20ce5a-92cf-4f33-b70f-c69b1df44a2e"},{"abstract":"$-1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 15/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 15/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 15/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 15/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 15/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150058","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150058,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150058,"related_publication":149530,"title":"Table 15","uuid":"ceff3865-271f-4f23-80f1-62d01e5a63da"},{"abstract":"Observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 16/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 16/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 16/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 16/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 16/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150059","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150059,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150059,"related_publication":149530,"title":"Table 16","uuid":"033981f8-2871-4ce2-b4a7-d0335ff12bed"},{"abstract":"$+1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 17/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 17/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 17/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 17/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 17/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150060","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150060,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150060,"related_publication":149530,"title":"Table 17","uuid":"7b6ade1b-8f7c-4f98-9e3e-c83675c28d45"},{"abstract":"$-1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 18/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 18/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 18/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 18/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 18/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150061","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150061,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150061,"related_publication":149530,"title":"Table 18","uuid":"1989e5aa-6c52-4ea7-918e-ae43ffcb6d93"},{"abstract":"Expected 95% CL exclusion limits on the simplified models of higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 19/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 19/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 19/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 19/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 19/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150062","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t19","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150062,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150062,"related_publication":149530,"title":"Table 19","uuid":"acba91ae-78a4-4aca-9cb9-81c1a9dfd7ae"},{"abstract":"$+1\\sigma$ expected 95% CL exclusion limits on the simplified models of higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 20/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 20/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 20/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 20/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 20/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150063","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t20","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150063,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150063,"related_publication":149530,"title":"Table 20","uuid":"f4701b16-72bd-4587-bfc1-a020ada536aa"},{"abstract":"$-1\\sigma$ expected 95% CL exclusion limits on the simplified models of higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 21/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 21/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 21/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 21/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 21/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150064","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t21","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150064,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150064,"related_publication":149530,"title":"Table 21","uuid":"85608027-18fa-4f09-9065-e8d545337906"},{"abstract":"Observed 95% CL exclusion limits on the simplified models of higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 22/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 22/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 22/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 22/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 22/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150065","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t22","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150065,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150065,"related_publication":149530,"title":"Table 22","uuid":"01758e0c-91f0-45e0-ba3b-eafe7ef30e2d"},{"abstract":"$+1\\sigma$ observed 95% CL exclusion limits on the simplified models of higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 23/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 23/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 23/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 23/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 23/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150066","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t23","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150066,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150066,"related_publication":149530,"title":"Table 23","uuid":"826c4aa1-c3b0-43c7-ae3f-dac241bc02ad"},{"abstract":"$-1\\sigma$ observed 95% CL exclusion limits on the simplified models of higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 24/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 24/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 24/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 24/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 24/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150067","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t24","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150067,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150067,"related_publication":149530,"title":"Table 24","uuid":"26bc8833-51bf-415e-9d89-12de8d15fe63"},{"abstract":"Observed upper limit on the signal cross section in fb for the production of $\\tilde{\\chi}_1^{+}\\tilde{\\chi}_{1}^{-}$.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 25/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 25/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 25/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 25/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 25/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150068","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t25","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150068,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"SIG"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150068,"related_publication":149530,"title":"Table 25","uuid":"5d3b4fce-2350-47f1-b87e-f5a10478cc1a"},{"abstract":"The analyses used in combination for each scenario to set limits in models of the production of $\\tilde{\\chi}_1^{+}\\tilde{\\chi}_{1}^{-}$.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 26/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 26/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 26/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 26/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 26/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150069","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino pair"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t26","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150069,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino pair"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150069,"related_publication":149530,"title":"Table 26","uuid":"90de42f4-0858-4db2-84f9-5871ffedf8fa"},{"abstract":"Observed upper limit on the signal cross section in fb for chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 27/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 27/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 27/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 27/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 27/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150070","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t27","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150070,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"SIG"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150070,"related_publication":149530,"title":"Table 27","uuid":"a091139b-9c76-4ec9-887b-441f20f6b8b5"},{"abstract":"The analyses used in combination for each scenario to set limits in models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 28/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 28/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 28/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 28/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 28/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150071","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t28","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150071,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150071,"related_publication":149530,"title":"Table 28","uuid":"56c20e03-b322-4135-b8ad-5ce14039e80d"},{"abstract":"Expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 29/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 29/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 29/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 29/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 29/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150072","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t29","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150072,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150072,"related_publication":149530,"title":"Table 29","uuid":"af649668-18fa-4235-aba0-3e8a5211d3aa"},{"abstract":"$+1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 30/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 30/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 30/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 30/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 30/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150073","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t30","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150073,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150073,"related_publication":149530,"title":"Table 30","uuid":"212070b2-9792-4a77-97cd-fd9dc056e917"},{"abstract":"$-1\\sigma$ expected 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 31/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 31/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 31/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 31/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 31/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150074","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t31","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150074,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150074,"related_publication":149530,"title":"Table 31","uuid":"becef62e-09e3-4347-9ea1-e568fb1d1dc2"},{"abstract":"Observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 32/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 32/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 32/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 32/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 32/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150075","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t32","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150075,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150075,"related_publication":149530,"title":"Table 32","uuid":"6669556f-60c6-416a-9f3c-432feef7345a"},{"abstract":"$+1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 33/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 33/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 33/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 33/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 33/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150076","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t33","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150076,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150076,"related_publication":149530,"title":"Table 33","uuid":"a29f1e39-60c2-4163-b990-daa56e0ec0b9"},{"abstract":"$-1\\sigma$ observed 95% CL exclusion limits on the simplified models of chargino--neutralino production decaying via W and Z bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 34/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 34/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 34/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 34/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 34/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150077","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t34","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150077,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150077,"related_publication":149530,"title":"Table 34","uuid":"6e63bd62-4b7b-47f1-8ded-8aa680df2e32"},{"abstract":"Observed upper limit on the signal cross section in fb for chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 35/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 35/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 35/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 35/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 35/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150078","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t35","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150078,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"SIG"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150078,"related_publication":149530,"title":"Table 35","uuid":"087cef6c-6ea2-4402-8aee-e46916fe4528"},{"abstract":"The analyses used in combination for each scenario to set limits in models of chargino--neutralino production decaying via W and h bosons.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 36/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 36/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 36/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 36/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 36/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150079","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t36","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150079,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> chargino-1 neutralino-2"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150079,"related_publication":149530,"title":"Table 36","uuid":"ffccf5e3-4136-4db7-99e1-fb1eb8d2befb"},{"abstract":"Observed upper limit on the signal cross section in fb for higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 37/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 37/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 37/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 37/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 37/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150080","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t37","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150080,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"SIG"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150080,"related_publication":149530,"title":"Table 37","uuid":"6f5dd675-a671-4f5d-ba17-9d9d00232cb8"},{"abstract":"The analyses used in combination for each scenario to set limits in higgsino GGM scenarios.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2758009/Table 38/csv","json":"https://www.hepdata.net/download/table/ins2758009/Table 38/json","root":"https://www.hepdata.net/download/table/ins2758009/Table 38/root","yaml":"https://www.hepdata.net/download/table/ins2758009/Table 38/yaml","yoda":"https://www.hepdata.net/download/table/ins2758009/Table 38/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150081","creation_date":"2024-02-13","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["SUSY","proton-proton scattering","Supersymmetry"],"reactions":["p p -> Higgsino GGM"]},"date":"13 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149530.v1/t38","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150081,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"p p -> Higgsino GGM"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"proton-proton scattering"}],"last_updated":"2024-03-18T15:37:06","parent_child_join":{"name":"child_datatable","parent":"149530"},"recid":150081,"related_publication":149530,"title":"Table 38","uuid":"a57e9a56-8090-431d-8a7f-853f3150b309"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS","N","SIG"],"phrases":["Supersymmetry","proton-proton scattering","SUSY"],"reactions":["p p -> Higgsino GGM","p p -> chargino pair","p p -> chargino-1 neutralino-2"]},"date":"13 Feb 2024","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.149530","id":149530,"inspire_id":"2758009","journal_info":"CERN-EP-2024-018","keywords":[{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"chargino: pair production"},{"schema":"INSPIRE","value":"Wino: pair production"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"neutralino: associated production"},{"schema":"INSPIRE","value":"chargino: associated production"},{"schema":"INSPIRE","value":"Higgsino: pair production"},{"schema":"INSPIRE","value":"decay modes"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"statistical analysis"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"sensitivity"},{"schema":"INSPIRE","value":"sparticle: mass: lower limit"},{"schema":"INSPIRE","value":"channel cross section: upper limit"},{"schema":"INSPIRE","value":"supersymmetry: parameter space"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-03-18T15:37:13","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-03-18T00:00:00","recid":149530,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"},{"affiliation":"INFN, Udine","full_name":"Acharya, Bobby Samir"}],"title":"A statistical combination of ATLAS Run 2 searches for charginos and neutralinos at the LHC","total_tables":38,"type":["article"],"uuid":"d5b90586-1e76-41c5-9373-f95e0c2f0879","version":1,"year":"2024"},{"abstract":"A summary of the constraints from searches performed by the ATLAS Collaboration for the electroweak production of charginos and neutralinos is presented. Results from eight separate ATLAS searches are considered, each using 140 fb$^{-1}$ of proton-proton data at a centre-of-mass energy of $\\sqrt{s}$=13 TeV collected at the Large Hadron Collider during its second data-taking run. The results are interpreted in the context of the 19-parameter phenomenological minimal supersymmetric standard model, where R-parity conservation is assumed and the lightest supersymmetric particle is assumed to be the lightest neutralino. Constraints from previous electroweak, flavour and dark matter related measurements are also considered. The results are presented in terms of constraints on supersymmetric particle masses and are compared with limits from simplified models. Also shown is the impact of ATLAS searches on parameters such as the dark matter relic density and the spin-dependent and spin-independent scattering cross-sections targeted by direct dark matter detection experiments. The Higgs boson and Z boson `funnel regions', where a low-mass neutralino would not oversaturate the dark matter relic abundance, are almost completely excluded by the considered constraints. Example spectra for non-excluded supersymmetric models with light charginos and neutralinos are also presented.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2755168/1/csv","json":"https://www.hepdata.net/download/submission/ins2755168/1/json","root":"https://www.hepdata.net/download/submission/ins2755168/1/root","yaml":"https://www.hepdata.net/download/submission/ins2755168/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2755168/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2402.01392","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"149493","creation_date":"2024-02-02","data":[{"abstract":"SLHA files and exclusion information (in CSV format) are available to download for the pMSSM models in this paper. Please refer to this web page for download links along with a description of the contents.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2755168/Model files/csv","json":"https://www.hepdata.net/download/table/ins2755168/Model files/json","root":"https://www.hepdata.net/download/table/ins2755168/Model files/root","yaml":"https://www.hepdata.net/download/table/ins2755168/Model files/yaml","yoda":"https://www.hepdata.net/download/table/ins2755168/Model files/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150597","creation_date":"2024-02-02","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["SUSY","pMSSM","Electroweak","Supersymmetry"]},"date":"02 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149493.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150597,"inspire_id":"2755168","journal_info":"CERN-EP-2024-021","keywords":[{"name":"phrases","synonyms":"","value":"pMSSM"},{"name":"phrases","synonyms":"","value":"Electroweak"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"cmenergies","synonyms":"","value":"13000.0"}],"last_updated":"2024-03-28T11:04:02","parent_child_join":{"name":"child_datatable","parent":"149493"},"recid":150597,"related_publication":149493,"title":"Model files","uuid":"2a6e2ac8-3c64-484b-b2c7-b4b887985032"},{"abstract":"SLHA files and exclusion information (in CSV format) are available to download for the pMSSM models in this paper. Please refer to this web page for download links along with a description of the contents.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2755168/Model exclusion/csv","json":"https://www.hepdata.net/download/table/ins2755168/Model exclusion/json","root":"https://www.hepdata.net/download/table/ins2755168/Model exclusion/root","yaml":"https://www.hepdata.net/download/table/ins2755168/Model exclusion/yaml","yoda":"https://www.hepdata.net/download/table/ins2755168/Model exclusion/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"150598","creation_date":"2024-02-02","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["SUSY","pMSSM","Electroweak","Supersymmetry"]},"date":"02 Feb 2024","doc_type":"datatable","doi":"10.17182/hepdata.149493.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":150598,"inspire_id":"2755168","journal_info":"CERN-EP-2024-021","keywords":[{"name":"phrases","synonyms":"","value":"pMSSM"},{"name":"phrases","synonyms":"","value":"Electroweak"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"cmenergies","synonyms":"","value":"13000.0"}],"last_updated":"2024-03-28T11:04:02","parent_child_join":{"name":"child_datatable","parent":"149493"},"recid":150598,"related_publication":149493,"title":"Model exclusion","uuid":"058efa0d-d688-46c1-94d6-1fa38f09a0b4"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Supersymmetry","pMSSM","Electroweak","SUSY"]},"date":"02 Feb 2024","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.149493","id":149493,"inspire_id":"2755168","journal_info":"CERN-EP-2024-021","keywords":[{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"dark matter: relic density"},{"schema":"INSPIRE","value":"spin: dependence"},{"schema":"INSPIRE","value":"sparticle: mass"},{"schema":"INSPIRE","value":"mass: lower limit"},{"schema":"INSPIRE","value":"dark matter: direct detection"},{"schema":"INSPIRE","value":"sparticle: pair production"},{"schema":"INSPIRE","value":"chargino: production"},{"schema":"INSPIRE","value":"neutralino: LSP"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"electroweak interaction"},{"schema":"INSPIRE","value":"R parity"},{"schema":"INSPIRE","value":"minimal supersymmetric standard model"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"supersymmetry: parameter space"},{"schema":"INSPIRE","value":"conservation law"},{"schema":"INSPIRE","value":"Higgs particle"},{"schema":"INSPIRE","value":"dark matter: scattering"},{"schema":"INSPIRE","value":"WIMP nucleon: cross section"},{"schema":"INSPIRE","value":"channel cross section: upper limit"},{"schema":"INSPIRE","value":"flavor"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-03-28T11:04:03","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-03-28T00:00:00","recid":149493,"subject_area":["hep-ex","Phenomenology-HEP","hep-ph"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"},{"affiliation":"INFN, Udine","full_name":"Acharya, Bobby Samir"}],"title":"ATLAS Run 2 searches for electroweak production of supersymmetric particles interpreted within the pMSSM","total_tables":2,"type":["article"],"uuid":"912e4c31-add6-4aa0-a58d-f43e5a7e7cb7","version":1,"year":"2024"},{"abstract":"This paper presents a search for pair production of higgsinos, the supersymmetric partners of the Higgs bosons, in scenarios with gauge-mediated supersymmetry breaking. Each higgsino is assumed to decay into a Higgs boson and a nearly massless gravitino. The search targets events where each Higgs boson decays into $b\\bar{b}$, leading to a reconstructed final state with at least three energetic $b$-jets and missing transverse momentum. Two complementary analysis channels are used, with each channel specifically targeting either low or high values of the higgsino mass. The low-mass (high-mass) channel exploits 126 (139) fb$^{-1}$ of $\\sqrt{s}=13$ TeV data collected by the ATLAS detector during Run 2 of the Large Hadron Collider. No significant excess above the Standard Model prediction is found. At 95% confidence level, masses between 130 GeV and 940 GeV are excluded for higgsinos decaying exclusively into Higgs bosons and gravitinos. Exclusion limits as a function of the higgsino decay branching ratio to a Higgs boson are also reported.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2751932/1/csv","json":"https://www.hepdata.net/download/submission/ins2751932/1/json","root":"https://www.hepdata.net/download/submission/ins2751932/1/root","yaml":"https://www.hepdata.net/download/submission/ins2751932/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2751932/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2401.14922","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"136030","creation_date":"2024-01-26","data":[{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 250 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 250 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 250 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 250 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 250 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146946","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146946,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146946,"related_publication":136030,"title":"Yield table for 250 GeV high-mass regions","uuid":"ef215fdd-688d-4dc4-b857-a8f1c61bc0ca"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 300 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 300 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 300 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 300 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 300 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146947","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146947,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146947,"related_publication":136030,"title":"Yield table for 300 GeV high-mass regions","uuid":"1f338309-17fa-4140-b14d-04c4497b6c18"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 400 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 400 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 400 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 400 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 400 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146948","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146948,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146948,"related_publication":136030,"title":"Yield table for 400 GeV high-mass regions","uuid":"58deb172-2f1b-43dc-acce-056e84be3fb5"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 500 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 500 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 500 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 500 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 500 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146949","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146949,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146949,"related_publication":136030,"title":"Yield table for 500 GeV high-mass regions","uuid":"651af9d8-2324-4936-bb1d-9ea8379eb905"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 600 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 600 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 600 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 600 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 600 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146950","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146950,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146950,"related_publication":136030,"title":"Yield table for 600 GeV high-mass regions","uuid":"eb9166d4-7074-41b3-bbe0-d334cd0b4eb5"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 700 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 700 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 700 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 700 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 700 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146951","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146951,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146951,"related_publication":136030,"title":"Yield table for 700 GeV high-mass regions","uuid":"ea2646b9-798d-4c95-b119-af3dc2bce791"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 800 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 800 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 800 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 800 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 800 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146952","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146952,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146952,"related_publication":136030,"title":"Yield table for 800 GeV high-mass regions","uuid":"aaea3464-15fc-4be0-b446-eb4139fd0b3f"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 900 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 900 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 900 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 900 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 900 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146953","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146953,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146953,"related_publication":136030,"title":"Yield table for 900 GeV high-mass regions","uuid":"bdb8380d-7d0b-458a-b21f-b1079fdac446"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1000 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1000 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1000 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1000 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1000 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146954","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146954,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146954,"related_publication":136030,"title":"Yield table for 1000 GeV high-mass regions","uuid":"9ce1f258-aa83-4d1c-ad7d-0e69aaafbc89"},{"abstract":"Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1100 GeV high-mass regions/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1100 GeV high-mass regions/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1100 GeV high-mass regions/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1100 GeV high-mass regions/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 1100 GeV high-mass regions/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146955","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146955,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146955,"related_publication":136030,"title":"Yield table for 1100 GeV high-mass regions","uuid":"adfcfe3a-9fb8-46ef-adc8-f797b2249dc2"},{"abstract":"Pre-fit data and background (reweighted $2b$) predictions for each $4b$ SR $E_\\text{T}^\\text{miss}$ and $m_\\text{eff}$ bin of the low-mass channel for the 2016 data-taking period. The bottom panel shows the significance of any differences between the observed $4b$ data and the background prediction. The $1\\sigma$ and $2\\sigma$ bands are shown in green and yellow, respectively. All systematics are included except the background normalization, which is 2.3%.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2016 low-mass exclusion region/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2016 low-mass exclusion region/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2016 low-mass exclusion region/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2016 low-mass exclusion region/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2016 low-mass exclusion region/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146956","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146956,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146956,"related_publication":136030,"title":"Yield table for 2016 low-mass exclusion region","uuid":"1ca07136-aaaa-4a05-ad4a-fab887decc3c"},{"abstract":"Pre-fit data and background (reweighted $2b$) predictions for each $4b$ SR $E_\\text{T}^\\text{miss}$ and $m_\\text{eff}$ bin of the low-mass channel for the 2017 data-taking period. The bottom panel shows the significance of any differences between the observed $4b$ data and the background prediction. The $1\\sigma$ and $2\\sigma$ bands are shown in green and yellow, respectively. All systematics are included except the background normalization, which is 3.7%.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2017 low-mass exclusion region/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2017 low-mass exclusion region/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2017 low-mass exclusion region/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2017 low-mass exclusion region/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2017 low-mass exclusion region/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146957","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146957,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146957,"related_publication":136030,"title":"Yield table for 2017 low-mass exclusion region","uuid":"2d9a28d8-4969-47e5-bea2-efcb5a9a8188"},{"abstract":"Pre-fit data and background (reweighted $2b$) predictions for each $4b$ SR $E_\\text{T}^\\text{miss}$ and $m_\\text{eff}$ bin of the low-mass channel for the 2018 data-taking period. The bottom panel shows the significance of any differences between the observed $4b$ data and the background prediction. The $1\\sigma$ and $2\\sigma$ bands are shown in green and yellow, respectively. All systematics are included except the background normalization, which is 1.8%.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2018 low-mass exclusion region/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2018 low-mass exclusion region/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2018 low-mass exclusion region/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2018 low-mass exclusion region/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for 2018 low-mass exclusion region/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146958","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146958,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146958,"related_publication":136030,"title":"Yield table for 2018 low-mass exclusion region","uuid":"5546f011-3395-4cba-aa03-2b8127744ac7"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Limits for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/Limits for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/Limits for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Limits for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Limits for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146959","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146959,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146959,"related_publication":136030,"title":"Limits for combined","uuid":"e6af56d0-0247-480e-bd00-861ae4a6f137"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146960","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146960,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146960,"related_publication":136030,"title":"+1$\\sigma$ limits for combined","uuid":"bf7d28ec-cb62-44f4-9587-80909b24ef49"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146961","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146961,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146961,"related_publication":136030,"title":"-1$\\sigma$ limits for combined","uuid":"03d47521-1f66-435f-9072-7ac1f5d4b8b6"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146962","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146962,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146962,"related_publication":136030,"title":"+2$\\sigma$ limits for combined","uuid":"8a00fdac-0028-42d8-972e-01ba9bb93de3"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146963","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146963,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146963,"related_publication":136030,"title":"-2$\\sigma$ limits for combined","uuid":"c117345a-0820-4e00-8270-7c9d9dad6897"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146964","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t19","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146964,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146964,"related_publication":136030,"title":"Limits over theory for combined","uuid":"5d6bf91c-e532-4124-bd2e-fe6461b0f4ea"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits over theory for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits over theory for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits over theory for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits over theory for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits over theory for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146965","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t20","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146965,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146965,"related_publication":136030,"title":"+1$\\sigma$ limits over theory for combined","uuid":"9724b8a3-e4bf-4206-ba0c-3bc04b62d398"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits over theory for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits over theory for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits over theory for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits over theory for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits over theory for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146966","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t21","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146966,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146966,"related_publication":136030,"title":"-1$\\sigma$ limits over theory for combined","uuid":"08efe05f-9f33-4615-8bab-e738db62a663"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits over theory for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits over theory for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits over theory for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits over theory for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits over theory for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146967","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t22","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146967,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146967,"related_publication":136030,"title":"+2$\\sigma$ limits over theory for combined","uuid":"193c2bb9-dd34-44b8-98d2-6178203d3af6"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. Results from a previous ATLAS search using 24.3-36.1 fb$^{-1}$ [13] are shown by the solid (observed) and dashed (expected) blue lines. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits over theory for combined/csv","json":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits over theory for combined/json","root":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits over theory for combined/root","yaml":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits over theory for combined/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits over theory for combined/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146968","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t23","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146968,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146968,"related_publication":136030,"title":"-2$\\sigma$ limits over theory for combined","uuid":"95c33971-5ae4-4dd4-9a4c-cbac84a68232"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the 95% CL observed (solid) and expected (dashed) upper limits on $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})$, assuming the theory cross section for higgsino pair production. The higgsinos are assumed to decay as $\\tilde{H}\\rightarrow h + \\tilde{G}$ or $\\tilde{H}\\rightarrow Z + \\tilde{G}$. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Limits for BR/csv","json":"https://www.hepdata.net/download/table/ins2751932/Limits for BR/json","root":"https://www.hepdata.net/download/table/ins2751932/Limits for BR/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Limits for BR/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Limits for BR/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146969","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t24","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146969,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146969,"related_publication":136030,"title":"Limits for BR","uuid":"db7a2295-c2df-49f8-a538-8d922adbf68e"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the 95% CL observed (solid) and expected (dashed) upper limits on $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})$, assuming the theory cross section for higgsino pair production. The higgsinos are assumed to decay as $\\tilde{H}\\rightarrow h + \\tilde{G}$ or $\\tilde{H}\\rightarrow Z + \\tilde{G}$. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for BR/csv","json":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for BR/json","root":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for BR/root","yaml":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for BR/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/+1$%5Csigma$ limits for BR/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146970","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t25","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146970,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146970,"related_publication":136030,"title":"+1$\\sigma$ limits for BR","uuid":"f0cc26cf-290f-45ee-a859-31d1c4daa01c"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the 95% CL observed (solid) and expected (dashed) upper limits on $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})$, assuming the theory cross section for higgsino pair production. The higgsinos are assumed to decay as $\\tilde{H}\\rightarrow h + \\tilde{G}$ or $\\tilde{H}\\rightarrow Z + \\tilde{G}$. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for BR/csv","json":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for BR/json","root":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for BR/root","yaml":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for BR/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/-1$%5Csigma$ limits for BR/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146971","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t26","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146971,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146971,"related_publication":136030,"title":"-1$\\sigma$ limits for BR","uuid":"f51f3083-2a95-41b3-8981-1cff1dd3163d"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the 95% CL observed (solid) and expected (dashed) upper limits on $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})$, assuming the theory cross section for higgsino pair production. The higgsinos are assumed to decay as $\\tilde{H}\\rightarrow h + \\tilde{G}$ or $\\tilde{H}\\rightarrow Z + \\tilde{G}$. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for BR/csv","json":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for BR/json","root":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for BR/root","yaml":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for BR/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/+2$%5Csigma$ limits for BR/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146972","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t27","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146972,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146972,"related_publication":136030,"title":"+2$\\sigma$ limits for BR","uuid":"83bac104-1d52-4afa-b7ca-7f8ed6c00a9f"},{"abstract":"Exclusion limits of the low-mass and high-mass channels. The low-mass channel is used for $m_{\\tilde{H}}<250$ GeV while the high-mass channel is used for $m_{\\tilde{H}}\\ge250$ GeV. The plot shows the 95% CL observed (solid) and expected (dashed) upper limits on $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})$, assuming the theory cross section for higgsino pair production. The higgsinos are assumed to decay as $\\tilde{H}\\rightarrow h + \\tilde{G}$ or $\\tilde{H}\\rightarrow Z + \\tilde{G}$. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for BR/csv","json":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for BR/json","root":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for BR/root","yaml":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for BR/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/-2$%5Csigma$ limits for BR/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146973","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t28","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146973,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146973,"related_publication":136030,"title":"-2$\\sigma$ limits for BR","uuid":"1ae23349-6641-451e-8fea-8942cf630544"},{"abstract":"Exclusion limits of the low-mass channel. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Limits for low-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Limits for low-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Limits for low-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Limits for low-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Limits for low-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146974","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t29","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146974,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146974,"related_publication":136030,"title":"Limits for low-mass","uuid":"0963de66-b2b2-432a-8436-5e4262c6295c"},{"abstract":"Exclusion limits of the low-mass channel. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for low-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for low-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for low-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for low-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for low-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146975","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t30","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146975,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146975,"related_publication":136030,"title":"Limits over theory for low-mass","uuid":"4fea70f0-54b7-4f87-be31-bf111951cbb1"},{"abstract":"Exclusion limits of the high-mass channel. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Limits for high-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Limits for high-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Limits for high-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Limits for high-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Limits for high-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146976","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t31","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146976,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146976,"related_publication":136030,"title":"Limits for high-mass","uuid":"f7d9e7fc-d02d-4652-b485-b93cdbf5548f"},{"abstract":"Exclusion limits of the high-mass channel. The plot shows the observed (solid) and expected (dashed) 95% CL upper limits on the cross section of higgsino pair production, assuming a higgsino decay branching ratio of $\\mathcal{B}(\\tilde{H}\\rightarrow h + \\tilde{G})=100\\%$. The theory cross section and its uncertainty are shown by the solid red line and red shading. The bottom panel shows the ratio of the limits to the theory cross section. The phase space above the lines is excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for high-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for high-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for high-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for high-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Limits over theory for high-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146977","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLs"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t32","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146977,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"observables","synonyms":"","value":"CLs"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146977,"related_publication":136030,"title":"Limits over theory for high-mass","uuid":"df01c89a-8304-41d6-bdcb-476053347b98"},{"abstract":"Results of the background-only fit in the low-mass channel discovery region SR_LM_150. Both pre-fit and post-fit values are shown.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_150/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_150/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_150/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_150/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_150/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146978","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t33","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146978,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146978,"related_publication":136030,"title":"Yield table for SR_LM_150","uuid":"774b2c8e-7595-4efc-997e-07f6e30b3613"},{"abstract":"Results of the background-only fit in the low-mass channel discovery region SR_LM_300. Both pre-fit and post-fit values are shown.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_300/csv","json":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_300/json","root":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_300/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_300/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Yield table for SR_LM_300/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146979","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t34","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146979,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146979,"related_publication":136030,"title":"Yield table for SR_LM_300","uuid":"e160d740-b921-4373-9866-f373096095a4"},{"abstract":"The experimental efficiency of the low-mass channel for the exclusion and discovery signal regions as a function of higgsino mass. The experimental efficiency is defined as the number of events passing the detector-level event selections divided by the number of events passing the event selections for a perfect detector. The denominator is obtained by implementing particle-level event selections that emulate the detector-level selections. This treats the lack of availability of $b$-jet triggers as an inefficiency.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Efficiency for low-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Efficiency for low-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Efficiency for low-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Efficiency for low-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Efficiency for low-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146980","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t35","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146980,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146980,"related_publication":136030,"title":"Efficiency for low-mass","uuid":"32a6b2c8-25bd-4c33-b734-6f048a96de03"},{"abstract":"The particle-level acceptance for the low-mass exclusion and discovery signal regions, shown as a function of higgsino mass. The acceptance is defined as the fraction of signal events passing the particle-level event selection that emulates the detector-level selection. The acceptance calculation considers only those signal events where both higgsinos decay to Higgs bosons.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Acceptance for low-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Acceptance for low-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Acceptance for low-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Acceptance for low-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Acceptance for low-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146981","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t36","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146981,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"ACC"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146981,"related_publication":136030,"title":"Acceptance for low-mass","uuid":"0b4fe3d1-442f-4024-821a-38ec0576ef8b"},{"abstract":"The experimental efficiency of the high-mass channel discovery regions as a function of higgsino mass. For each higgsino mass, the efficiency is shown for the SR-1 region corresponding to the mass. For masses above 1100 GeV, SR-1-1100 is used. The experimental efficiency is defined as the number of events passing the detector-level event selections divided by the number of events passing the event selections for a perfect detector. The denominator is obtained by implementing particle-level event selections that emulate the detector-level selections. The efficiency calculation considers only those signal events where both higgsinos decay to Higgs bosons.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Efficiency for high-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Efficiency for high-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Efficiency for high-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Efficiency for high-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Efficiency for high-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146982","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t37","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146982,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146982,"related_publication":136030,"title":"Efficiency for high-mass","uuid":"1c169e8e-8022-4e21-a03f-2163284929d1"},{"abstract":"The particle-level acceptance for the high-mass signal regions, shown as a function of higgsino mass. For each higgsino mass, the acceptance is shown for the SR-1 region corresponding to the mass. For masses above 1100 GeV, SR-1-1100 is used. The acceptance is defined as the fraction of signal events passing the particle-level event selection that emulates the detector-level selection. The acceptance calculation considers only those signal events where both higgsinos decay to Higgs bosons.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Acceptance for high-mass/csv","json":"https://www.hepdata.net/download/table/ins2751932/Acceptance for high-mass/json","root":"https://www.hepdata.net/download/table/ins2751932/Acceptance for high-mass/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Acceptance for high-mass/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Acceptance for high-mass/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146983","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t38","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146983,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"ACC"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146983,"related_publication":136030,"title":"Acceptance for high-mass","uuid":"ff27cf27-a3b1-4356-b62a-ce07df2b7455"},{"abstract":"Cutflow for the low-mass channel for a representative 130 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 130 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 130 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 130 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 130 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 130 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146984","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t39","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146984,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146984,"related_publication":136030,"title":"Cutflow for low-mass 130 GeV sample","uuid":"b5c420b0-5826-4d62-b35c-abc07f35b0de"},{"abstract":"Cutflow for the low-mass channel for a representative 150 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 150 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 150 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 150 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 150 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 150 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146985","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t40","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146985,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146985,"related_publication":136030,"title":"Cutflow for low-mass 150 GeV sample","uuid":"bcdb68d9-fb8c-41a0-a95c-e26fdab8c9ed"},{"abstract":"Cutflow for the low-mass channel for a representative 200 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 200 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 200 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 200 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 200 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 200 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146986","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t41","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146986,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146986,"related_publication":136030,"title":"Cutflow for low-mass 200 GeV sample","uuid":"3505f7eb-cb7e-44d9-ad74-0c12bb5db033"},{"abstract":"Cutflow for the low-mass channel for a representative 250 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 250 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 250 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 250 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 250 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 250 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146987","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t42","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146987,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146987,"related_publication":136030,"title":"Cutflow for low-mass 250 GeV sample","uuid":"8884b058-2d7d-470e-8fab-39ba7e21efd4"},{"abstract":"Cutflow for the low-mass channel for a representative 300 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 300 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 300 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 300 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 300 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 300 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146988","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t43","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146988,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146988,"related_publication":136030,"title":"Cutflow for low-mass 300 GeV sample","uuid":"c806bde5-0efb-461d-bbaa-7f28def996a6"},{"abstract":"Cutflow for the low-mass channel for a representative 400 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 400 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 400 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 400 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 400 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 400 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146989","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t44","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146989,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146989,"related_publication":136030,"title":"Cutflow for low-mass 400 GeV sample","uuid":"54e6c55f-4393-4f7d-bcbf-f5b4a082948e"},{"abstract":"Cutflow for the low-mass channel for a representative 500 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 500 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 500 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 500 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 500 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 500 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146990","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t45","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146990,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146990,"related_publication":136030,"title":"Cutflow for low-mass 500 GeV sample","uuid":"2e550d19-a45b-4ab8-ac1f-29591961e1ae"},{"abstract":"Cutflow for the low-mass channel for a representative 600 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 600 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 600 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 600 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 600 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 600 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146991","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t46","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146991,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146991,"related_publication":136030,"title":"Cutflow for low-mass 600 GeV sample","uuid":"7646a2bc-d0d9-4995-ada1-d74f935ce921"},{"abstract":"Cutflow for the low-mass channel for a representative 700 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 700 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 700 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 700 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 700 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 700 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146992","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t47","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146992,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146992,"related_publication":136030,"title":"Cutflow for low-mass 700 GeV sample","uuid":"6f938c2a-18b4-4a56-a721-ffd4bd4b6548"},{"abstract":"Cutflow for the low-mass channel for a representative 800 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 800 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 800 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 800 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 800 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 800 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146993","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t48","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146993,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146993,"related_publication":136030,"title":"Cutflow for low-mass 800 GeV sample","uuid":"f6e39b43-9916-4cbf-9614-3c3489cb3cc3"},{"abstract":"Cutflow for the low-mass channel for a representative 900 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 900 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 900 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 900 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 900 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 900 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146994","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t49","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146994,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146994,"related_publication":136030,"title":"Cutflow for low-mass 900 GeV sample","uuid":"4dc5f958-eb10-4831-b875-06db70b65ef9"},{"abstract":"Cutflow for the low-mass channel for a representative 1000 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1000 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1000 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1000 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1000 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1000 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146995","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t50","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146995,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146995,"related_publication":136030,"title":"Cutflow for low-mass 1000 GeV sample","uuid":"a4320139-b4b5-4b4f-8609-8277384ed2e2"},{"abstract":"Cutflow for the low-mass channel for a representative 1100 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. The $b$-jet cut requires 4 or more $b$-jets with $p_\\text{T}>40$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$, with the availability of $b$-jet triggers lowering the luminosity to 126 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1100 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1100 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1100 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1100 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for low-mass 1100 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146996","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t51","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146996,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146996,"related_publication":136030,"title":"Cutflow for low-mass 1100 GeV sample","uuid":"cf3a8648-e81e-4f30-8248-73f5c0f55ea9"},{"abstract":"Cutflow for the high-mass channel for a representative 200 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 200 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 200 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 200 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 200 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 200 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146997","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t52","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146997,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146997,"related_publication":136030,"title":"Cutflow for high-mass 200 GeV sample","uuid":"5603529a-fa0d-4f38-8ef3-2a197caa9153"},{"abstract":"Cutflow for the high-mass channel for a representative 250 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 250 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 250 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 250 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 250 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 250 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146998","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t53","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146998,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146998,"related_publication":136030,"title":"Cutflow for high-mass 250 GeV sample","uuid":"5e6d13e2-f9cd-4b24-aa5f-aadf7acc7253"},{"abstract":"Cutflow for the high-mass channel for a representative 300 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 300 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 300 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 300 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 300 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 300 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"146999","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t54","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":146999,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":146999,"related_publication":136030,"title":"Cutflow for high-mass 300 GeV sample","uuid":"ce024768-9f5c-4527-ba8d-b18057ba4f1a"},{"abstract":"Cutflow for the high-mass channel for a representative 400 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 400 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 400 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 400 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 400 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 400 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147000","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t55","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147000,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147000,"related_publication":136030,"title":"Cutflow for high-mass 400 GeV sample","uuid":"234c2fa7-6b95-4fa1-a721-377b564e7ed7"},{"abstract":"Cutflow for the high-mass channel for a representative 500 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 500 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 500 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 500 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 500 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 500 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147001","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t56","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147001,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"},{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147001,"related_publication":136030,"title":"Cutflow for high-mass 500 GeV sample","uuid":"312f29ee-354d-49bc-8435-d72e6d6fcad9"},{"abstract":"Cutflow for the high-mass channel for a representative 600 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 600 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 600 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 600 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 600 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 600 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147002","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t57","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147002,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147002,"related_publication":136030,"title":"Cutflow for high-mass 600 GeV sample","uuid":"c27ec49c-80c9-414e-a76e-a2867e3aaa15"},{"abstract":"Cutflow for the high-mass channel for a representative 700 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 700 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 700 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 700 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 700 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 700 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147003","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t58","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147003,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147003,"related_publication":136030,"title":"Cutflow for high-mass 700 GeV sample","uuid":"0e1b481b-3ff5-42f2-ad1d-81fe73578a1a"},{"abstract":"Cutflow for the high-mass channel for a representative 800 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 800 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 800 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 800 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 800 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 800 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147004","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t59","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147004,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147004,"related_publication":136030,"title":"Cutflow for high-mass 800 GeV sample","uuid":"9a11d6ce-aeba-46f1-a71f-2b87fc9f21d1"},{"abstract":"Cutflow for the high-mass channel for a representative 900 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 900 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 900 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 900 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 900 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 900 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147005","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t60","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147005,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147005,"related_publication":136030,"title":"Cutflow for high-mass 900 GeV sample","uuid":"d598a3ae-818a-4797-bc96-5ed909b4b16d"},{"abstract":"Cutflow for the high-mass channel for a representative 1000 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1000 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1000 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1000 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1000 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1000 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147006","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t61","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147006,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147006,"related_publication":136030,"title":"Cutflow for high-mass 1000 GeV sample","uuid":"47aef5ed-92f2-4e75-9733-4dda5e2ee3a9"},{"abstract":"Cutflow for the high-mass channel for a representative 1100 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1100 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1100 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1100 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1100 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1100 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147007","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t62","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147007,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147007,"related_publication":136030,"title":"Cutflow for high-mass 1100 GeV sample","uuid":"8e01d008-2a36-4a04-9e58-7c08c677f184"},{"abstract":"Cutflow for the high-mass channel for a representative 1200 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1200 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1200 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1200 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1200 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1200 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147008","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t63","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147008,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147008,"related_publication":136030,"title":"Cutflow for high-mass 1200 GeV sample","uuid":"5a6a7f2e-333b-4de2-bff2-61560245cab4"},{"abstract":"Cutflow for the high-mass channel for a representative 1300 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1300 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1300 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1300 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1300 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1300 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147009","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t64","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147009,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147009,"related_publication":136030,"title":"Cutflow for high-mass 1300 GeV sample","uuid":"b3eed4fe-67ce-4a76-816f-c6e2ce65371b"},{"abstract":"Cutflow for the high-mass channel for a representative 1400 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1400 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1400 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1400 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1400 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1400 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147010","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t65","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147010,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147010,"related_publication":136030,"title":"Cutflow for high-mass 1400 GeV sample","uuid":"246b2933-81c7-44e6-a8fe-62e1ace03edc"},{"abstract":"Cutflow for the high-mass channel for a representative 1500 GeV signal. The preselection requires 4 or more jets with $p_\\text{T}>25$ GeV and 2 or more $b$-jets with $p_\\text{T}>25$ GeV. As the samples are generated with $\\mathcal{B}(\\tilde{H}\\rightarrow h\\tilde{G})$=50%, $\\mathcal{B}(\\tilde{H}\\rightarrow Z\\tilde{G})$=50% to allow for both decays to be studied, the $hh$ events selection is used to select the events where each of the higgsinos decays to a Higgs boson. Expected yields are normalized to a luminosity of 139 fb$^{-1}$. All selections are cumulative, with the exception of the SR cuts, which are each applied separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1500 GeV sample/csv","json":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1500 GeV sample/json","root":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1500 GeV sample/root","yaml":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1500 GeV sample/yaml","yoda":"https://www.hepdata.net/download/table/ins2751932/Cutflow for high-mass 1500 GeV sample/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147011","creation_date":"2024-01-26","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.136030.v1/t66","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147011,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"name":"observables","synonyms":"","value":"N"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Higgs"},{"name":"phrases","synonyms":"","value":"Higgs pair Production"},{"name":"phrases","synonyms":"","value":"Beauty"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO"}],"last_updated":"2024-02-05T11:53:26","parent_child_join":{"name":"child_datatable","parent":"136030"},"recid":147011,"related_publication":136030,"title":"Cutflow for high-mass 1500 GeV sample","uuid":"4aea0a63-fb6c-4c3f-81c7-b5bd84d168b1"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF","CLs","N","ACC"],"phrases":["Higgsino","Proton-Proton","Beauty","SUSY","Higgs","Higgs pair Production","Supersymmetry"],"reactions":["P P --> HIGGSINO"]},"date":"26 Jan 2024","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.136030","id":136030,"inspire_id":"2751932","journal_info":"CERN-EP-2023-278","keywords":[{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"new physics: search for"},{"schema":"INSPIRE","value":"Higgsino: pair production"},{"schema":"INSPIRE","value":"Higgsino: decay modes"},{"schema":"INSPIRE","value":"Higgsino: mass"},{"schema":"INSPIRE","value":"transverse momentum: missing-energy"},{"schema":"INSPIRE","value":"gravitino: massless"},{"schema":"INSPIRE","value":"supersymmetry: symmetry breaking"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"Higgs particle: hadronic decay"},{"schema":"INSPIRE","value":"bottom: pair production"},{"schema":"INSPIRE","value":"final state: ((n)jet)"},{"schema":"INSPIRE","value":"jet: bottom"},{"schema":"INSPIRE","value":"bottom: particle identification"},{"schema":"INSPIRE","value":"Higgs particle: pair production"},{"schema":"INSPIRE","value":"gravitation"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"Higgsino: branching ratio"},{"schema":"INSPIRE","value":"mass: lower limit"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-02-05T11:53:37","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-02-28T00:00:00","recid":136030,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"},{"affiliation":"INFN, Udine","full_name":"Acharya, Bobby Samir"}],"title":"Search for pair production of higgsinos in events with two Higgs bosons and missing transverse momentum in $\\sqrt{s}=13$ TeV $pp$ collisions at the ATLAS experiment","total_tables":66,"type":["article"],"uuid":"0c07201f-070e-49c6-8bb4-f8023b3ce370","version":1,"year":"2024"},{"abstract":"Higgsinos with masses near the electroweak scale can solve the hierarchy problem and provide a dark matter candidate, while detecting them at the LHC remains challenging if their mass-splitting is $\\mathcal{O}$(1 GeV). This Letter presents a novel search for nearly mass-degenerate higgsinos in events with an energetic jet, missing transverse momentum, and a low-momentum track with a significant transverse impact parameter using 140 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}$ = 13 TeV collected by the ATLAS experiment. For the first time since LEP, a range of mass-splittings between the lightest charged and neutral higgsinos from 0.3 GeV to 0.9 GeV is excluded at 95% confidence level, with a maximum reach of approximately 170 GeV in the higgsino mass.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2751400/1/csv","json":"https://www.hepdata.net/download/submission/ins2751400/1/json","root":"https://www.hepdata.net/download/submission/ins2751400/1/root","yaml":"https://www.hepdata.net/download/submission/ins2751400/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2751400/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2401.14046","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboelela, Mohammed","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso"],"collaborations":["ATLAS"],"control_number":"146944","creation_date":"2024-01-25","data":[{"abstract":"Number of expected and observed data events in the SR (top), and the model-independent upper limits obtained from their consistency (bottom). The symbol $\\tau_{\\ell}$ ($\\tau_{h}$) refers to fully-leptonic (hadron-involved) tau decays. The Others category includes contributions from minor background processes including $t\\bar{t}$, single-top and diboson. The individual uncertainties can be correlated and do not necessarily sum up in quadrature to the total uncertainty. The bottom section shows the observed 95% CL upper limits on the visible cross-section ($\\langle\\epsilon\\sigma\\rangle_{\\mathrm{obs}}^{95}$), on the number of generic signal events ($S_{\\mathrm{obs}}^{95}$) as well as the expected limit ($S_{\\mathrm{exp}}^{95}$) given the expected number (and $\\pm 1\\sigma$ deviations from the expectation) of background events.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/SR Yields Table/csv","json":"https://www.hepdata.net/download/table/ins2751400/SR Yields Table/json","root":"https://www.hepdata.net/download/table/ins2751400/SR Yields Table/root","yaml":"https://www.hepdata.net/download/table/ins2751400/SR Yields Table/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/SR Yields Table/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147319","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147319,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"N"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147319,"related_publication":146944,"title":"SR Yields Table","uuid":"c3456cd6-13ac-4e2a-a59b-858211c4d48b"},{"abstract":"Expected (dashed black line) and observed (solid red line) 95% CL exclusion limits on the higgsino simplified model being considered. These are shown with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively. The limits set by the latest ATLAS searches using the soft lepton and disappearing track signatures are illustrated by the blue and green regions, respectively, while the limit imposed by the LEP experiments is shown in gray. The dot-dashed gray line indicates the predicted mass-splitting for the pure higgsino scenario.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Expected exclusion limits from Figure 3/csv","json":"https://www.hepdata.net/download/table/ins2751400/Expected exclusion limits from Figure 3/json","root":"https://www.hepdata.net/download/table/ins2751400/Expected exclusion limits from Figure 3/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Expected exclusion limits from Figure 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Expected exclusion limits from Figure 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147320","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147320,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147320,"related_publication":146944,"title":"Expected exclusion limits from Figure 3","uuid":"8f16f0f8-ea88-4818-9f6e-70b47c9231be"},{"abstract":"Expected (dashed black line) and observed (solid red line) 95% CL exclusion limits on the higgsino simplified model being considered. These are shown with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively. The limits set by the latest ATLAS searches using the soft lepton and disappearing track signatures are illustrated by the blue and green regions, respectively, while the limit imposed by the LEP experiments is shown in gray. The dot-dashed gray line indicates the predicted mass-splitting for the pure higgsino scenario.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Expected $+1%5Csigma$ exclusion limits from Figure 3/csv","json":"https://www.hepdata.net/download/table/ins2751400/Expected $+1%5Csigma$ exclusion limits from Figure 3/json","root":"https://www.hepdata.net/download/table/ins2751400/Expected $+1%5Csigma$ exclusion limits from Figure 3/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Expected $+1%5Csigma$ exclusion limits from Figure 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Expected $+1%5Csigma$ exclusion limits from Figure 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147321","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147321,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147321,"related_publication":146944,"title":"Expected $+1\\sigma$ exclusion limits from Figure 3","uuid":"f4805894-0b05-420b-ae11-ee0c5a20e75e"},{"abstract":"Expected (dashed black line) and observed (solid red line) 95% CL exclusion limits on the higgsino simplified model being considered. These are shown with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively. The limits set by the latest ATLAS searches using the soft lepton and disappearing track signatures are illustrated by the blue and green regions, respectively, while the limit imposed by the LEP experiments is shown in gray. The dot-dashed gray line indicates the predicted mass-splitting for the pure higgsino scenario.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Expected $-1%5Csigma$ exclusion limits from Figure 3/csv","json":"https://www.hepdata.net/download/table/ins2751400/Expected $-1%5Csigma$ exclusion limits from Figure 3/json","root":"https://www.hepdata.net/download/table/ins2751400/Expected $-1%5Csigma$ exclusion limits from Figure 3/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Expected $-1%5Csigma$ exclusion limits from Figure 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Expected $-1%5Csigma$ exclusion limits from Figure 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147322","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147322,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147322,"related_publication":146944,"title":"Expected $-1\\sigma$ exclusion limits from Figure 3","uuid":"da845bcd-cc20-4d9a-a7b0-b75588e4fbc8"},{"abstract":"Expected (dashed black line) and observed (solid red line) 95% CL exclusion limits on the higgsino simplified model being considered. These are shown with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively. The limits set by the latest ATLAS searches using the soft lepton and disappearing track signatures are illustrated by the blue and green regions, respectively, while the limit imposed by the LEP experiments is shown in gray. The dot-dashed gray line indicates the predicted mass-splitting for the pure higgsino scenario.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Observed exclusion limits from Figure 3/csv","json":"https://www.hepdata.net/download/table/ins2751400/Observed exclusion limits from Figure 3/json","root":"https://www.hepdata.net/download/table/ins2751400/Observed exclusion limits from Figure 3/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Observed exclusion limits from Figure 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Observed exclusion limits from Figure 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147323","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147323,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147323,"related_publication":146944,"title":"Observed exclusion limits from Figure 3","uuid":"30266aa1-34c9-4ccd-bb23-ffd6b633f742"},{"abstract":"Expected (dashed black line) and observed (solid red line) 95% CL exclusion limits on the higgsino simplified model being considered. These are shown with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively. The limits set by the latest ATLAS searches using the soft lepton and disappearing track signatures are illustrated by the blue and green regions, respectively, while the limit imposed by the LEP experiments is shown in gray. The dot-dashed gray line indicates the predicted mass-splitting for the pure higgsino scenario.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Observed $+1%5Csigma$ exclusion limits from Figure 3/csv","json":"https://www.hepdata.net/download/table/ins2751400/Observed $+1%5Csigma$ exclusion limits from Figure 3/json","root":"https://www.hepdata.net/download/table/ins2751400/Observed $+1%5Csigma$ exclusion limits from Figure 3/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Observed $+1%5Csigma$ exclusion limits from Figure 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Observed $+1%5Csigma$ exclusion limits from Figure 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147324","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147324,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147324,"related_publication":146944,"title":"Observed $+1\\sigma$ exclusion limits from Figure 3","uuid":"747a5eb2-57da-42b8-ade1-71db806198ba"},{"abstract":"Expected (dashed black line) and observed (solid red line) 95% CL exclusion limits on the higgsino simplified model being considered. These are shown with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively. The limits set by the latest ATLAS searches using the soft lepton and disappearing track signatures are illustrated by the blue and green regions, respectively, while the limit imposed by the LEP experiments is shown in gray. The dot-dashed gray line indicates the predicted mass-splitting for the pure higgsino scenario.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Observed $-1%5Csigma$ exclusion limits from Figure 3/csv","json":"https://www.hepdata.net/download/table/ins2751400/Observed $-1%5Csigma$ exclusion limits from Figure 3/json","root":"https://www.hepdata.net/download/table/ins2751400/Observed $-1%5Csigma$ exclusion limits from Figure 3/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Observed $-1%5Csigma$ exclusion limits from Figure 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Observed $-1%5Csigma$ exclusion limits from Figure 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147325","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147325,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147325,"related_publication":146944,"title":"Observed $-1\\sigma$ exclusion limits from Figure 3","uuid":"841eeb70-7b98-4295-bb54-994a169d3e42"},{"abstract":"Expected and observed CLs values per signal point represented by the grey numbers. The expected (dashed) and observed (solid) 95% CL exclusion limits are overlaid along with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Expected CLs values from Figure 3a/csv","json":"https://www.hepdata.net/download/table/ins2751400/Expected CLs values from Figure 3a/json","root":"https://www.hepdata.net/download/table/ins2751400/Expected CLs values from Figure 3a/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Expected CLs values from Figure 3a/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Expected CLs values from Figure 3a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147326","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147326,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147326,"related_publication":146944,"title":"Expected CLs values from Figure 3a","uuid":"12c27506-f5be-4a76-a9db-5f48b8df8482"},{"abstract":"Expected and observed CLs values per signal point represented by the grey numbers. The expected (dashed) and observed (solid) 95% CL exclusion limits are overlaid along with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Observed CLs values from Figure 3b/csv","json":"https://www.hepdata.net/download/table/ins2751400/Observed CLs values from Figure 3b/json","root":"https://www.hepdata.net/download/table/ins2751400/Observed CLs values from Figure 3b/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Observed CLs values from Figure 3b/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Observed CLs values from Figure 3b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147327","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147327,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147327,"related_publication":146944,"title":"Observed CLs values from Figure 3b","uuid":"b92ad209-23b4-4395-98f8-6aff2c7f3cc4"},{"abstract":"Expected and observed cross-section upper-limit per signal point represented by the grey numbers. The expected (dashed) and observed (solid) 95% CL exclusion limits are overlaid along with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Expected cross-section upper-limits from Figure 4a/csv","json":"https://www.hepdata.net/download/table/ins2751400/Expected cross-section upper-limits from Figure 4a/json","root":"https://www.hepdata.net/download/table/ins2751400/Expected cross-section upper-limits from Figure 4a/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Expected cross-section upper-limits from Figure 4a/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Expected cross-section upper-limits from Figure 4a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147328","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG","CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147328,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"observables","synonyms":"","value":"SIG"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147328,"related_publication":146944,"title":"Expected cross-section upper-limits from Figure 4a","uuid":"d5bcbfa0-53e6-41bc-8676-7c1b7669eb03"},{"abstract":"Expected and observed cross-section upper-limit per signal point represented by the grey numbers. The expected (dashed) and observed (solid) 95% CL exclusion limits are overlaid along with $\\pm 1\\sigma_{\\mathrm{exp}}$ (yellow band) from experimental systematic and statistical uncertainties, and with $\\pm 1\\sigma_{\\mathrm{theory}}^{\\mathrm{SUSY}}$ (red dotted lines) from signal cross-section uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Observed cross-section upper-limits from Figure 4b/csv","json":"https://www.hepdata.net/download/table/ins2751400/Observed cross-section upper-limits from Figure 4b/json","root":"https://www.hepdata.net/download/table/ins2751400/Observed cross-section upper-limits from Figure 4b/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Observed cross-section upper-limits from Figure 4b/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Observed cross-section upper-limits from Figure 4b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147329","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG","CLS"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147329,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"observables","synonyms":"","value":"SIG"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147329,"related_publication":146944,"title":"Observed cross-section upper-limits from Figure 4b","uuid":"dcf6837f-4661-45b6-8dfd-0e1f332dd060"},{"abstract":"Truth-level signal acceptances for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$) in a SR with the $S(d_0)$ requirement removed. The acceptance is defined as the fraction of accepted events divided by the total number of events in the generator-level signal Monte Carlo simulation, where the signal candidate track is identified as the charged particle with the largest distance between the interaction vertex and the secondary vertex of the higgsino decays.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$/csv","json":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$/json","root":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147330","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147330,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"ACC"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147330,"related_publication":146944,"title":"Signal acceptances for $\\tilde{\\chi}_1^- \\tilde{\\chi}_1^0$","uuid":"82f562bc-8557-42b9-9ca2-6b1d9dc97bea"},{"abstract":"Truth-level signal acceptances for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$) in a SR with the $S(d_0)$ requirement removed. The acceptance is defined as the fraction of accepted events divided by the total number of events in the generator-level signal Monte Carlo simulation, where the signal candidate track is identified as the charged particle with the largest distance between the interaction vertex and the secondary vertex of the higgsino decays.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$/csv","json":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$/json","root":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147331","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147331,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"ACC"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147331,"related_publication":146944,"title":"Signal acceptances for $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^0$","uuid":"499ecae6-27fa-4e37-9246-fa439b5e5f35"},{"abstract":"Truth-level signal acceptances for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$) in a SR with the $S(d_0)$ requirement removed. The acceptance is defined as the fraction of accepted events divided by the total number of events in the generator-level signal Monte Carlo simulation, where the signal candidate track is identified as the charged particle with the largest distance between the interaction vertex and the secondary vertex of the higgsino decays.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$/csv","json":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$/json","root":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147332","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147332,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"ACC"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147332,"related_publication":146944,"title":"Signal acceptances for $\\tilde{\\chi}_1^- \\tilde{\\chi}_2^0$","uuid":"83edf921-34d7-4864-8ded-4d5fb2c6bb59"},{"abstract":"Truth-level signal acceptances for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$) in a SR with the $S(d_0)$ requirement removed. The acceptance is defined as the fraction of accepted events divided by the total number of events in the generator-level signal Monte Carlo simulation, where the signal candidate track is identified as the charged particle with the largest distance between the interaction vertex and the secondary vertex of the higgsino decays.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$/csv","json":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$/json","root":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147333","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147333,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"ACC"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147333,"related_publication":146944,"title":"Signal acceptances for $\\tilde{\\chi}_1^+ \\tilde{\\chi}_2^0$","uuid":"3f02db7b-ac8a-4961-bad9-4f88989f4b06"},{"abstract":"Truth-level signal acceptances for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$) in a SR with the $S(d_0)$ requirement removed. The acceptance is defined as the fraction of accepted events divided by the total number of events in the generator-level signal Monte Carlo simulation, where the signal candidate track is identified as the charged particle with the largest distance between the interaction vertex and the secondary vertex of the higgsino decays.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$/csv","json":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$/json","root":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147334","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147334,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"ACC"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147334,"related_publication":146944,"title":"Signal acceptances for $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$","uuid":"6e8a58d7-8cfa-4989-8b8e-86d8e9153a54"},{"abstract":"Truth-level signal acceptances for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$) in a SR with the $S(d_0)$ requirement removed. The acceptance is defined as the fraction of accepted events divided by the total number of events in the generator-level signal Monte Carlo simulation, where the signal candidate track is identified as the charged particle with the largest distance between the interaction vertex and the secondary vertex of the higgsino decays.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_1^2$/csv","json":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_1^2$/json","root":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_1^2$/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_1^2$/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Signal acceptances for $%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_1^2$/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147335","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147335,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"ACC"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147335,"related_publication":146944,"title":"Signal acceptances for $\\tilde{\\chi}_1^0 \\tilde{\\chi}_1^2$","uuid":"3b5a55d0-1766-443d-8c3c-9c482a1bb7be"},{"abstract":"Signal efficiencies in SR-Low for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147336","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147336,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147336,"related_publication":146944,"title":"$\\tilde{\\chi}_1^- \\tilde{\\chi}_1^0$ SR-Low signal efficiencies","uuid":"bd34d3a2-889d-48c5-a484-3d9d39f3502e"},{"abstract":"Signal efficiencies in SR-Low for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-Low signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147337","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t19","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147337,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147337,"related_publication":146944,"title":"$\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^0$ SR-Low signal efficiencies","uuid":"3534a8d5-9102-491d-8b89-093a528df76c"},{"abstract":"Signal efficiencies in SR-Low for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147338","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t20","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147338,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147338,"related_publication":146944,"title":"$\\tilde{\\chi}_1^- \\tilde{\\chi}_2^0$ SR-Low signal efficiencies","uuid":"a82ff7c0-b045-410d-9369-4cebb21dcb3a"},{"abstract":"Signal efficiencies in SR-Low for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147339","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t21","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147339,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147339,"related_publication":146944,"title":"$\\tilde{\\chi}_1^+ \\tilde{\\chi}_2^0$ SR-Low signal efficiencies","uuid":"a11b87bf-5828-45ef-a2fe-c004e2ccceb2"},{"abstract":"Signal efficiencies in SR-Low for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-Low signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-Low signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-Low signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-Low signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-Low signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147340","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t22","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147340,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147340,"related_publication":146944,"title":"$\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$ SR-Low signal efficiencies","uuid":"1eea8b70-f3d6-4f81-a8c9-bb5899e8fc11"},{"abstract":"Signal efficiencies in SR-Low for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-Low signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147341","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t23","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147341,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147341,"related_publication":146944,"title":"$\\tilde{\\chi}_1^0 \\tilde{\\chi}_2^0$ SR-Low signal efficiencies","uuid":"8a55d2cf-2ad3-4961-a29a-30105f42a24c"},{"abstract":"Signal efficiencies in SR-High for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147342","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t24","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147342,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147342,"related_publication":146944,"title":"$\\tilde{\\chi}_1^- \\tilde{\\chi}_1^0$ SR-High signal efficiencies","uuid":"b0e33671-4c83-4121-915f-d5de7ee4556e"},{"abstract":"Signal efficiencies in SR-High for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^0$ SR-High signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147343","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t25","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147343,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147343,"related_publication":146944,"title":"$\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^0$ SR-High signal efficiencies","uuid":"5776e2bb-d85e-4ec0-b283-d83ef4df3eb0"},{"abstract":"Signal efficiencies in SR-High for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^- %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147344","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t26","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147344,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147344,"related_publication":146944,"title":"$\\tilde{\\chi}_1^- \\tilde{\\chi}_2^0$ SR-High signal efficiencies","uuid":"b4e4e6ed-e5a8-4b45-8675-401b57c434ba"},{"abstract":"Signal efficiencies in SR-High for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147345","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t27","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147345,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147345,"related_publication":146944,"title":"$\\tilde{\\chi}_1^+ \\tilde{\\chi}_2^0$ SR-High signal efficiencies","uuid":"51e93ace-7fd9-49c3-929a-496622ecc21a"},{"abstract":"Signal efficiencies in SR-High for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-High signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-High signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-High signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-High signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^+ %5Ctilde{%5Cchi}_1^-$ SR-High signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147346","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t28","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147346,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147346,"related_publication":146944,"title":"$\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$ SR-High signal efficiencies","uuid":"adab38ef-4fb0-4bc0-a472-71073c0204f4"},{"abstract":"Signal efficiencies in SR-High for each production process ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$), defined by the number of events of reconstructed-level signal simulation divided by the number of events obtained at generator level, where the $S(d_0)$ selecton efficiency has the largest impact. The higgsino decay products from $\\Delta \\mathrm{m}(\\tilde{\\chi}_1^\\pm,\\tilde{\\chi}_1^0) < 0.4$ GeV signal have $p_{\\mathrm{T}}$ too low to be reconstructed as the signal candidate tracks, and therefore the identified signal candidate tracks are typically from pile-up collisions or underlying events similar to the QCD track background, causing a low $S(d_0)$ selection efficiency in these plots.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/json","root":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/$%5Ctilde{%5Cchi}_1^0 %5Ctilde{%5Cchi}_2^0$ SR-High signal efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147347","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t29","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147347,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147347,"related_publication":146944,"title":"$\\tilde{\\chi}_1^0 \\tilde{\\chi}_2^0$ SR-High signal efficiencies","uuid":"3e977f41-d872-43a6-9115-b4ad55b29822"},{"abstract":"Event selection cutflows for signal samples with $m(\\tilde{\\chi}_{1}^0)$ = 150 GeV and $\\Delta m(\\tilde{\\chi}_{1}^\\pm, \\tilde{\\chi}_{1}^0)$ = 1.5, 1.0, and 0.75 GeV, including all six production processes ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$). The cross-section used to obtain the initial number of events ($\\sigma(\\mathrm{n}_{\\mathrm{jets}}) \\geq 1$) refers to an emission of at least one gluon or quark with $p_{\\mathrm{T}} > 50$ GeV at the parton level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 1/csv","json":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 1/json","root":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147348","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t30","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147348,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"N"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147348,"related_publication":146944,"title":"Cutflows Table 1","uuid":"9c1e652e-179d-48c1-aa0a-1f988a914507"},{"abstract":"Event selection cutflows for signal samples with $m(\\tilde{\\chi}_{1}^0)$ = 150 GeV and $\\Delta m(\\tilde{\\chi}_{1}^\\pm, \\tilde{\\chi}_{1}^0)$ = 0.5, 0.35, and 0.25 GeV, including all six production processes ($\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_1^0$, $\\tilde{\\chi}_1^\\pm \\tilde{\\chi}_2^0$, $\\tilde{\\chi}_1^+ \\tilde{\\chi}_1^-$, and $\\tilde{\\chi}_2^0 \\tilde{\\chi}_1^0$). The cross-section used to obtain the initial number of events ($\\sigma(\\mathrm{n}_{\\mathrm{jets}}) \\geq 1$) refers to an emission of at least one gluon or quark with $p_{\\mathrm{T}} > 50$ GeV at the parton level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 2/csv","json":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 2/json","root":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2751400/Cutflows Table 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147349","creation_date":"2024-01-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["N"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.146944.v1/t31","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147349,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGSINO HIGGSINO JET"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Supersymmetry"},{"name":"phrases","synonyms":"","value":"SUSY"},{"name":"phrases","synonyms":"","value":"Higgsino"},{"name":"phrases","synonyms":"","value":"Displaced Tracks"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"N"}],"last_updated":"2024-02-21T16:46:05","parent_child_join":{"name":"child_datatable","parent":"146944"},"recid":147349,"related_publication":146944,"title":"Cutflows Table 2","uuid":"34c8fa5b-0c4a-48b8-85a8-5916f9a4ea9b"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF","N","ACC","CLS","SIG"],"phrases":["Displaced Tracks","SUSY","Higgsino","Supersymmetry","Proton-Proton Scattering"],"reactions":["P P --> HIGGSINO HIGGSINO JET"]},"date":"25 Jan 2024","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.146944","id":146944,"inspire_id":"2751400","journal_info":"CERN-EP-2024-012","keywords":[{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"transverse momentum: missing-energy"},{"schema":"INSPIRE","value":"scale: electroweak interaction"},{"schema":"INSPIRE","value":"tracks"},{"schema":"INSPIRE","value":"mass difference"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"dark matter: direct detection"},{"schema":"INSPIRE","value":"CERN LEP Stor"},{"schema":"INSPIRE","value":"transverse"},{"schema":"INSPIRE","value":"hierarchy"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"Higgsino: mass"},{"schema":"INSPIRE","value":"impact parameter"},{"schema":"INSPIRE","value":"track data analysis"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-02-21T16:46:11","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-02-28T00:00:00","recid":146944,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Southern Methodist U.","full_name":"Aboelela, Mohammed"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"}],"title":"Search for nearly mass-degenerate higgsinos using low-momentum mildly-displaced tracks in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","total_tables":31,"type":["article"],"uuid":"44f9c475-f2a7-4e67-9b2e-68d3d1efafa7","version":1,"year":"2024"},{"abstract":"A search for a new heavy boson produced via gluon-fusion in the four-lepton channel with missing transverse momentum or jets is performed. The search uses proton-proton collision data equivalent to an integrated luminosity of 139 fb$^{-1}$ at a centre-of-mass energy of 13 TeV collected by the ATLAS detector between 2015 and 2018 at the Large Hadron Collider. This study explores the decays of heavy bosons: $R\\rightarrow SH$ and $A\\rightarrow ZH$, where $R$ is a CP-even boson, $A$ is a CP-odd boson, $H$ is a CP-even boson, and $S$ is considered to decay into invisible particles that are candidates for dark matter. In these processes, $S\\rightarrow \\textrm{invisible}$ and $H\\rightarrow ZZ$. The $Z$ boson associated with the heavy scalar boson $H$ decays into all decay channels of the $Z$ boson. The mass range under consideration is 390-1300 (320-1300) GeV for the $R$ ($A$) boson and 220-1000 GeV for the $H$ boson. No significant deviation from the Standard Model backgrounds is observed. The results are interpreted as upper limits at a 95% confidence level on the cross-section times the branching ratio of the heavy resonances.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2745376/1/csv","json":"https://www.hepdata.net/download/submission/ins2745376/1/json","root":"https://www.hepdata.net/download/submission/ins2745376/1/root","yaml":"https://www.hepdata.net/download/submission/ins2745376/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2745376/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2401.04742","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming"],"collaborations":["ATLAS"],"control_number":"145687","creation_date":"2024-01-09","data":[{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search for SR1 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{R}, m_{H}) = (500, 300)$ GeV signal is normalised to the observed upper limit on the cross-section (25.0 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $R%5Cto SH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $R%5Cto SH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $R%5Cto SH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $R%5Cto SH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $R%5Cto SH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147216","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM+S"],"reactions":["P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147216,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- DM DMBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM+S"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147216,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR1 for $R\\to SH$ signal","uuid":"06d4eb42-0818-4416-bac7-deafdd07786d"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search for SR2 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{R}, m_{H}) = (500, 300)$ GeV signal is normalised to the observed upper limit on the cross-section (25.0 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $R%5Cto SH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $R%5Cto SH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $R%5Cto SH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $R%5Cto SH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $R%5Cto SH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147217","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM+S"],"reactions":["P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147217,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- DM DMBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM+S"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147217,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR2 for $R\\to SH$ signal","uuid":"149b76b8-48d6-4595-a2e0-ffbd71982d85"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search for SR3 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{R}, m_{H}) = (500, 300)$ GeV signal is normalised to the observed upper limit on the cross-section (25.0 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $R%5Cto SH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $R%5Cto SH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $R%5Cto SH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $R%5Cto SH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $R%5Cto SH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147218","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM+S"],"reactions":["P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147218,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- DM DMBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM+S"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147218,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR3 for $R\\to SH$ signal","uuid":"75775936-371c-4ef9-86b8-793552bb33b4"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR1 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{A}, m_{H}) = (510, 380)$ GeV signal is normalised to the observed upper limit on the cross-section (29.9 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $A%5Cto ZH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $A%5Cto ZH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $A%5Cto ZH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $A%5Cto ZH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR1 for $A%5Cto ZH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147219","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147219,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147219,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR1 for $A\\to ZH$ signal","uuid":"18e5fc71-e42c-4097-9467-3d3cc324794f"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR2 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{A}, m_{H}) = (510, 380)$ GeV signal is normalised to the observed upper limit on the cross-section (29.9 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $A%5Cto ZH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $A%5Cto ZH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $A%5Cto ZH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $A%5Cto ZH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR2 for $A%5Cto ZH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147220","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147220,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147220,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR2 for $A\\to ZH$ signal","uuid":"5f66825a-c624-428e-92fa-e65a566373f7"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR3 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{A}, m_{H}) = (510, 380)$ GeV signal is normalised to the observed upper limit on the cross-section (29.9 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $A%5Cto ZH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $A%5Cto ZH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $A%5Cto ZH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $A%5Cto ZH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR3 for $A%5Cto ZH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147221","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147221,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147221,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR3 for $A\\to ZH$ signal","uuid":"172b1a21-add7-45f3-9e78-8ff4a2e06b3b"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR4 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{A}, m_{H}) = (510, 380)$ GeV signal is normalised to the observed upper limit on the cross-section (29.9 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR4 for $A%5Cto ZH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR4 for $A%5Cto ZH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR4 for $A%5Cto ZH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR4 for $A%5Cto ZH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR4 for $A%5Cto ZH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147222","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147222,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147222,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR4 for $A\\to ZH$ signal","uuid":"5c08724d-1556-4ccd-b0cb-7b26141bf31a"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR5 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{A}, m_{H}) = (510, 380)$ GeV signal is normalised to the observed upper limit on the cross-section (29.9 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR5 for $A%5Cto ZH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR5 for $A%5Cto ZH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR5 for $A%5Cto ZH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR5 for $A%5Cto ZH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR5 for $A%5Cto ZH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147223","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147223,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147223,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR5 for $A\\to ZH$ signal","uuid":"8d074440-e5d9-4dbe-861c-efd5a1f2a146"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR6 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{A}, m_{H}) = (510, 380)$ GeV signal is normalised to the observed upper limit on the cross-section (29.9 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR6 for $A%5Cto ZH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR6 for $A%5Cto ZH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR6 for $A%5Cto ZH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR6 for $A%5Cto ZH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR6 for $A%5Cto ZH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147224","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147224,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147224,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR6 for $A\\to ZH$ signal","uuid":"05072f3e-f007-432e-b3b1-41c9550f3a48"},{"abstract":"Observed and expected distributions of the invariant mass of the four-lepton system in the $A\\to ZH\\to 4\\ell+X$ search for SR7 under a background-only fit to data. The total background includes the $q\\overline{q}\\to ZZ$, $gg\\to ZZ$, $q\\overline{q}\\to ZZ$ (EW), $VVV$, $t\\overline{t}V$, $t\\overline{t}$, $Z$+jets and $WZ$ processes. The distribution of the $(m_{A}, m_{H}) = (510, 380)$ GeV signal is normalised to the observed upper limit on the cross-section (29.9 fb).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR7 for $A%5Cto ZH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR7 for $A%5Cto ZH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR7 for $A%5Cto ZH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR7 for $A%5Cto ZH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Post-fit $m_{4%5Cell}$ in SR7 for $A%5Cto ZH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147225","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147225,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"m4l"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147225,"related_publication":145687,"title":"Post-fit $m_{4\\ell}$ in SR7 for $A\\to ZH$ signal","uuid":"850c286b-bd92-4758-86f5-19dd1fdf0706"},{"abstract":"Local p0-values in the $(m_{H}, m_{R})$ plane for the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search with $m_{S} = 160$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value for the $R%5Cto SH$ search/csv","json":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value for the $R%5Cto SH$ search/json","root":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value for the $R%5Cto SH$ search/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value for the $R%5Cto SH$ search/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value for the $R%5Cto SH$ search/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147226","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["p0-values"],"phrases":["2HDM+S"],"reactions":["P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147226,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- DM DMBAR"},{"name":"observables","synonyms":"","value":"p0-values"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM+S"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147226,"related_publication":145687,"title":"Observed local $p_{0}$-value for the $R\\to SH$ search","uuid":"8b2291d0-7fcd-4d3f-b2e3-441e009a3c74"},{"abstract":"Local p0-values in the $(m_{H}, m_{A})$ plane for the $A\\to ZH\\to 4\\ell+X$ search.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value the $A%5Cto ZH$ search/csv","json":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value the $A%5Cto ZH$ search/json","root":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value the $A%5Cto ZH$ search/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value the $A%5Cto ZH$ search/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Observed local $p_{0}$-value the $A%5Cto ZH$ search/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147227","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["p0-values"],"phrases":["2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147227,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"p0-values"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147227,"related_publication":145687,"title":"Observed local $p_{0}$-value the $A\\to ZH$ search","uuid":"c8a150ea-a36f-4455-9877-f3accca15a1a"},{"abstract":"The observed upper limits at 95% confidence level on $\\sigma(gg\\to R)\\times \\mathcal{B}(R\\to SH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{R})$ plane with $m_{S} = 160$ GeV for the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $R$ production/csv","json":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $R$ production/json","root":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $R$ production/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $R$ production/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $R$ production/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147228","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["cross-section limits","2HDM+S"],"reactions":["P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147228,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- DM DMBAR"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"cross-section limits"},{"name":"phrases","synonyms":"","value":"2HDM+S"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147228,"related_publication":145687,"title":"Observed upper limit on the cross-section for the $R$ production","uuid":"01e56daa-a964-43ef-8f2d-e4dd04548909"},{"abstract":"The expected upper limits at 95% confidence level on $\\sigma(gg\\to R)\\times \\mathcal{B}(R\\to SH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{R})$ plane with $m_{S} = 160$ GeV for the $R\\to SH\\to 4\\ell+E^{\\textrm{miss}}_{\\textrm{T}}$ search.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for the $R$ production/csv","json":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for the $R$ production/json","root":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for the $R$ production/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for the $R$ production/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for the $R$ production/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147229","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["cross-section limits","2HDM+S"],"reactions":["P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147229,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- DM DMBAR"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"cross-section limits"},{"name":"phrases","synonyms":"","value":"2HDM+S"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147229,"related_publication":145687,"title":"Expected upper limit on the cross-section for the $R$ production","uuid":"dcf7a583-f03f-4b46-b29a-01be5e6a1352"},{"abstract":"The observed upper limits at 95% confidence level on $\\sigma(gg\\to A)\\times \\mathcal{B}(A\\to ZH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{A})$ plane for the $A\\to ZH\\to 4\\ell+X$ search.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $A$ production/csv","json":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $A$ production/json","root":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $A$ production/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $A$ production/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Observed upper limit on the cross-section for the $A$ production/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147230","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["cross-section limits","2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147230,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"cross-section limits"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147230,"related_publication":145687,"title":"Observed upper limit on the cross-section for the $A$ production","uuid":"8a1c803b-7340-4666-9f8d-96e31a772fb5"},{"abstract":"The expected upper limits at 95% confidence level on $\\sigma(gg\\to A)\\times \\mathcal{B}(A\\to ZH)\\times (H\\to ZZ)$ across the $(m_{H}, m_{A})$ plane for the $A\\to ZH\\to 4\\ell+X$ search.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for $A$ production/csv","json":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for $A$ production/json","root":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for $A$ production/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for $A$ production/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Expected upper limit on the cross-section for $A$ production/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147231","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["cross-section limits","2HDM"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147231,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"cross-section limits"},{"name":"phrases","synonyms":"","value":"2HDM"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147231,"related_publication":145687,"title":"Expected upper limit on the cross-section for $A$ production","uuid":"925a747a-975c-4681-8135-082bf1874c1a"},{"abstract":"Cut-flow of the raw events at each selection stage for the $R\\rightarrow SH\\rightarrow 4\\ell + E^{\\textrm{miss}}_{\\textrm{T}}$ signal with a mass point of $(m_R, m_H ) = (390, 220)$ GeV and $m_S = 160$ GeV. The events are shown for the individual and combined four-lepton channels. The SFOS denotes same flavour and opposite sign lepton pairs selection and the final selection is shown for each signal region. The final selection criteria for SR1 to SR3 are defined in Table 2 of the paper.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Cut-flow table for the $R%5Cto SH$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Cut-flow table for the $R%5Cto SH$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Cut-flow table for the $R%5Cto SH$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Cut-flow table for the $R%5Cto SH$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Cut-flow table for the $R%5Cto SH$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147232","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147232,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- DM DMBAR"},{"name":"cmenergies","synonyms":"","value":"13000.0"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147232,"related_publication":145687,"title":"Cut-flow table for the $R\\to SH$ signal","uuid":"f1d8110f-eca7-4be4-9842-3a386a9fa12b"},{"abstract":"Cut-flow of the raw events at each selection stage for the $A\\rightarrow Z(\\rightarrow jj/\\ell^+\\ell^-/\\textrm{invisible})H(\\rightarrow 4\\ell)$ signal with a mass point of $(m_A, m_H ) = (330, 220)$ GeV. The events are shown for the individual and combined four-lepton channels. The SFOS denotes same flavour and opposite sign lepton pairs selection and the final selection is shown for each signal region. The final selection criteria for SR1 to SR7 are defined in Table 2 of the paper.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(jj/2%5Cell/%5Crm invisible)H(4%5Cell)$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(jj/2%5Cell/%5Crm invisible)H(4%5Cell)$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(jj/2%5Cell/%5Crm invisible)H(4%5Cell)$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(jj/2%5Cell/%5Crm invisible)H(4%5Cell)$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(jj/2%5Cell/%5Crm invisible)H(4%5Cell)$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147233","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147233,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"cmenergies","synonyms":"","value":"13000.0"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147233,"related_publication":145687,"title":"Cut-flow for the $A\\to Z(jj/2\\ell/\\rm invisible)H(4\\ell)$ signal","uuid":"b105fc16-1e60-4d6b-8036-3a4f1c587ae7"},{"abstract":"Cut-flow of the raw events at each selection stage for the $A\\rightarrow Z(\\rightarrow 2\\ell)H(\\rightarrow 2\\ell+jj/\\textrm{invisible})$ signal with a mass point of $(m_A, m_H ) = (330, 220)$ GeV. The events are shown for the individual and combined four-lepton channels. The SFOS denotes same flavour and opposite sign lepton pairs selection and the final selection is shown for each signal region. The final selection criteria for SR1 to SR7 are defined in Table 2 of the paper.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(2%5Cell)H(2%5Cell/jj/%5Crm invisible)$ signal/csv","json":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(2%5Cell)H(2%5Cell/jj/%5Crm invisible)$ signal/json","root":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(2%5Cell)H(2%5Cell/jj/%5Crm invisible)$ signal/root","yaml":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(2%5Cell)H(2%5Cell/jj/%5Crm invisible)$ signal/yaml","yoda":"https://www.hepdata.net/download/table/ins2745376/Cut-flow for the $A%5Cto Z(2%5Cell)H(2%5Cell/jj/%5Crm invisible)$ signal/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147234","creation_date":"2024-01-09","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"]},"date":"09 Jan 2024","doc_type":"datatable","doi":"10.17182/hepdata.145687.v1/t19","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147234,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"name":"reactions","synonyms":"","value":"P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR"},{"name":"cmenergies","synonyms":"","value":"13000.0"}],"last_updated":"2024-02-13T14:03:25","parent_child_join":{"name":"child_datatable","parent":"145687"},"recid":147234,"related_publication":145687,"title":"Cut-flow for the $A\\to Z(2\\ell)H(2\\ell/jj/\\rm invisible)$ signal","uuid":"9c970490-4461-4382-8477-ae76c31bb335"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["m4l","p0-values","CLS"],"phrases":["2HDM","2HDM+S","cross-section limits"],"reactions":["P P --> L+ L- L+ L- NU NU / L+ L- L+ L- Q QBAR","P P --> L+ L- L+ L- DM DMBAR"]},"date":"09 Jan 2024","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.145687","id":145687,"inspire_id":"2745376","journal_info":"CERN-EP-2023-291","keywords":[{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"gluon gluon: fusion"},{"schema":"INSPIRE","value":"resonance: production"},{"schema":"INSPIRE","value":"resonance: heavy"},{"schema":"INSPIRE","value":"transverse momentum: missing-energy"},{"schema":"INSPIRE","value":"boson: heavy"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"boson: scalar"},{"schema":"INSPIRE","value":"invisible decay"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"channel cross section: branching ratio: upper limit"},{"schema":"INSPIRE","value":"dark matter"},{"schema":"INSPIRE","value":"final state: (4lepton)"},{"schema":"INSPIRE","value":"final state: ((n)jet 4lepton)"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"background"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-02-13T14:03:28","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-02-13T00:00:00","recid":145687,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"}],"title":"Search for heavy resonances in final states with four leptons and missing transverse momentum or jets in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","total_tables":19,"type":["article"],"uuid":"5c524b83-b706-424d-8f17-4b9abc6740c3","version":1,"year":"2024"},{"abstract":"Following the first science results of the LUX-ZEPLIN (LZ) experiment, a dual-phase xenon time projection chamber operating from the Sanford Underground Research Facility in Lead, South Dakota, USA, we report the initial limits on a model-independent non-relativistic effective field theory describing the complete set of possible interactions of a weakly interacting massive particle (WIMP) with a nucleon. These results utilize the same 5.5 t fiducial mass and 60 live days of exposure collected for the LZ spin-independent and spin-dependent analyses while extending the upper limit of the energy region of interest by a factor of 7.5 to 270 keVnr. No significant excess in this high energy region is observed. Using a profile-likelihood ratio analysis, we report 90% confidence level exclusion limits on the coupling of each individual non-relativistic WIMP-nucleon operator for both elastic and inelastic interactions in the isoscalar and isovector bases.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2729878/1/csv","json":"https://www.hepdata.net/download/submission/ins2729878/1/json","root":"https://www.hepdata.net/download/submission/ins2729878/1/root","yaml":"https://www.hepdata.net/download/submission/ins2729878/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2729878/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2312.02030","authors":["Aalbers, J.","Akerib, D.S.","Musalhi, A.K. Al","Alder, F.","Amarasinghe, C.S.","Ames, A.","Anderson, T.J.","Angelides, N.","Ara\u00fajo, H.M.","Armstrong, J.E."],"collaborations":["LZ"],"control_number":"145873","creation_date":"2023-12-04","data":[{"abstract":"Data points used in analysis in log_10(S2)-S1 space.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/SR1 Data/csv","json":"https://www.hepdata.net/download/table/ins2729878/SR1 Data/json","root":"https://www.hepdata.net/download/table/ins2729878/SR1 Data/root","yaml":"https://www.hepdata.net/download/table/ins2729878/SR1 Data/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/SR1 Data/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146558","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["S1c (phd)","log10(S2c) (phd)"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t1","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146558,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"S1c (phd)"},{"name":"observables","synonyms":"","value":"log10(S2c) (phd)"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146558,"related_publication":145873,"title":"SR1 Data","uuid":"48336155-ccbe-4dc3-a4b3-706e1db44daf"},{"abstract":"Data selection efficiency as a function of nuclear recoil energy","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Nuclear Recoil Efficiency/csv","json":"https://www.hepdata.net/download/table/ins2729878/Nuclear Recoil Efficiency/json","root":"https://www.hepdata.net/download/table/ins2729878/Nuclear Recoil Efficiency/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Nuclear Recoil Efficiency/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Nuclear Recoil Efficiency/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146559","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Efficiency (%)"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t2","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146559,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Efficiency (%)"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146559,"related_publication":145873,"title":"Nuclear Recoil Efficiency","uuid":"3d032d74-13ba-41a5-a4e2-265678d0e725"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 8","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146560","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t3","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146560,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146560,"related_publication":145873,"title":"Operator 8 elastic isoscalar","uuid":"0a8c88f6-9501-4eba-a935-c5ee70097cb6"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 9","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146561","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t4","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146561,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146561,"related_publication":145873,"title":"Operator 9 elastic isoscalar","uuid":"8885534b-4c88-4355-ad94-49a2cff924d7"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 12","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146562","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t5","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146562,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146562,"related_publication":145873,"title":"Operator 12 elastic isoscalar","uuid":"5b443bbd-3028-46cd-be80-6b534b1459a2"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 7","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146563","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t6","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146563,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146563,"related_publication":145873,"title":"Operator 7 elastic isoscalar","uuid":"3ff505b5-609d-4f67-9cbe-8555d555bc50"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 13","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146564","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t7","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146564,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146564,"related_publication":145873,"title":"Operator 13 elastic isoscalar","uuid":"4d12266d-e1ad-4b91-8a55-706a7a2a420b"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 3","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146565","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t8","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146565,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146565,"related_publication":145873,"title":"Operator 3 elastic isoscalar","uuid":"8dd7adaa-5905-4c2f-9dfa-9c89ba68fed2"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 5","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146566","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t9","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146566,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146566,"related_publication":145873,"title":"Operator 5 elastic isoscalar","uuid":"d2e9b8e6-f53b-46d9-a184-0702e12197bd"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 11","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146567","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t10","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146567,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146567,"related_publication":145873,"title":"Operator 11 elastic isoscalar","uuid":"c079f4d0-35c2-4a07-a7ca-b5fa171dbbe2"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 14","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146568","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t11","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146568,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146568,"related_publication":145873,"title":"Operator 14 elastic isoscalar","uuid":"defcd2b9-d129-40fe-a504-541995ccf23e"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 4","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146569","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t12","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146569,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146569,"related_publication":145873,"title":"Operator 4 elastic isoscalar","uuid":"03525bc4-86c2-4217-ac14-4951ab86556e"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 10","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146570","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t13","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146570,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146570,"related_publication":145873,"title":"Operator 10 elastic isoscalar","uuid":"6577c967-ce74-487b-91cc-cc9f65c80a2a"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 1","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146571","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t14","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146571,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146571,"related_publication":145873,"title":"Operator 1 elastic isoscalar","uuid":"ad0c24a7-9480-4fda-bf26-8fe7287d8c81"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 6","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146572","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t15","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146572,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146572,"related_publication":145873,"title":"Operator 6 elastic isoscalar","uuid":"2466ccc4-c10a-4a9c-a04f-432e92400f7e"},{"abstract":"Isoscalar WIMP-nucleon elastic coupling limit for Operator 15","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146573","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t16","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146573,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146573,"related_publication":145873,"title":"Operator 15 elastic isoscalar","uuid":"a148de06-f595-444e-8404-517f8de810ce"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 3","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 3 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146574","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t17","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146574,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146574,"related_publication":145873,"title":"Operator 3 elastic isovector","uuid":"7d4b6272-e62c-480f-b6fe-d3039ea70c5b"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 10","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 10 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146575","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t18","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146575,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146575,"related_publication":145873,"title":"Operator 10 elastic isovector","uuid":"70c6be6b-0e71-4418-921f-ec23d7580f24"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 13","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 13 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146576","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t19","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146576,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146576,"related_publication":145873,"title":"Operator 13 elastic isovector","uuid":"4937e4c5-4f5a-41cf-a018-388fd2c2a9aa"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 12","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 12 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146577","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t20","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146577,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146577,"related_publication":145873,"title":"Operator 12 elastic isovector","uuid":"ad84f7ac-5a8a-4e9f-baca-b3215a57ca0e"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 8","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 8 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146578","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t21","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146578,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146578,"related_publication":145873,"title":"Operator 8 elastic isovector","uuid":"41c866e1-61b0-4685-a9b1-bb17dfca175a"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 1","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 1 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146579","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t22","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146579,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146579,"related_publication":145873,"title":"Operator 1 elastic isovector","uuid":"25bc7467-a2f6-4d04-82f3-0c8075647068"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 4","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 4 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146580","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t23","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146580,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146580,"related_publication":145873,"title":"Operator 4 elastic isovector","uuid":"fafd3697-0cd6-488a-90d1-ab5b85afc531"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 5","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 5 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146581","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t24","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146581,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146581,"related_publication":145873,"title":"Operator 5 elastic isovector","uuid":"9e124145-635f-4b98-b01c-3ed03ed3624d"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 7","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 7 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146582","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t25","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146582,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146582,"related_publication":145873,"title":"Operator 7 elastic isovector","uuid":"29d6c86d-2e71-47cd-b3e8-91574a638934"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 11","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 11 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146583","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t26","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146583,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146583,"related_publication":145873,"title":"Operator 11 elastic isovector","uuid":"732cb3bd-1bfe-4067-a1dd-e43ed18eae42"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 15","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 15 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146584","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t27","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146584,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146584,"related_publication":145873,"title":"Operator 15 elastic isovector","uuid":"df1be2ea-25f4-4bf9-b1cc-556d05530557"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 9","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 9 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146585","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t28","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146585,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146585,"related_publication":145873,"title":"Operator 9 elastic isovector","uuid":"8de66324-08ee-4a17-b7d2-8fcbf685abce"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 14","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 14 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146586","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t29","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146586,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146586,"related_publication":145873,"title":"Operator 14 elastic isovector","uuid":"f7e5668e-1ee9-4f32-af8a-81c59a5632de"},{"abstract":"Isovector WIMP-nucleon elastic coupling limit for Operator 6","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 6 elastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146587","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t30","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146587,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146587,"related_publication":145873,"title":"Operator 6 elastic isovector","uuid":"399552d9-e948-4980-8f85-9c3892fa05f5"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 12","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146588","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t31","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146588,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146588,"related_publication":145873,"title":"Operator 12 inelastic isoscalar","uuid":"e474c53c-cf86-471d-a1cd-9a17834b4208"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 3","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146589","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t32","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146589,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146589,"related_publication":145873,"title":"Operator 3 inelastic isoscalar","uuid":"182c2a9a-271c-452f-b31b-886ee6598299"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 9","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146590","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t33","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146590,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146590,"related_publication":145873,"title":"Operator 9 inelastic isoscalar","uuid":"5aaf1954-0f72-4656-b9fb-07ff32a9e038"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 7","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146591","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t34","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146591,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146591,"related_publication":145873,"title":"Operator 7 inelastic isoscalar","uuid":"f1efaa65-d939-4359-af15-acc46a23da52"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 10","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146592","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t35","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146592,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146592,"related_publication":145873,"title":"Operator 10 inelastic isoscalar","uuid":"6fabc614-139f-42a5-830c-848bf48e71c3"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 15","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146593","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t36","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146593,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146593,"related_publication":145873,"title":"Operator 15 inelastic isoscalar","uuid":"38a513c5-0e54-48bc-8fbd-fae5afb579d9"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 8","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146594","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t37","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146594,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146594,"related_publication":145873,"title":"Operator 8 inelastic isoscalar","uuid":"ff3f7096-e4c8-45ff-b712-80344b404b1d"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 4","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146595","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t38","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146595,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146595,"related_publication":145873,"title":"Operator 4 inelastic isoscalar","uuid":"3fd7b217-8f88-4332-ae47-3cbd7ece9f18"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 5","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146596","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t39","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146596,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146596,"related_publication":145873,"title":"Operator 5 inelastic isoscalar","uuid":"f02ba527-496a-4b06-bdd2-828a0433756b"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 6","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146597","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t40","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146597,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146597,"related_publication":145873,"title":"Operator 6 inelastic isoscalar","uuid":"b8141bee-1e4b-4a5f-a993-911f49686a41"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 13","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146598","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t41","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146598,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146598,"related_publication":145873,"title":"Operator 13 inelastic isoscalar","uuid":"049104c8-1c34-4b5a-8e6d-1f29cd52a6a8"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 11","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146599","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t42","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146599,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146599,"related_publication":145873,"title":"Operator 11 inelastic isoscalar","uuid":"5e2c6d19-903a-4510-b231-c04ad4d8dbb3"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 14","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146600","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t43","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146600,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146600,"related_publication":145873,"title":"Operator 14 inelastic isoscalar","uuid":"794b64c7-971d-4689-9f7d-6bfc077f4040"},{"abstract":"Isoscalar WIMP-nucleon inelastic coupling limit for Operator 1","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isoscalar/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isoscalar/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isoscalar/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isoscalar/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isoscalar/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146601","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t44","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146601,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146601,"related_publication":145873,"title":"Operator 1 inelastic isoscalar","uuid":"91bdff41-6560-4ef6-96d9-de0da2ec5334"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 13","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 13 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146602","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t45","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146602,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146602,"related_publication":145873,"title":"Operator 13 inelastic isovector","uuid":"f68a67a6-fadd-4b98-8678-1aedd000a948"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 1","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 1 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146603","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t46","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146603,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146603,"related_publication":145873,"title":"Operator 1 inelastic isovector","uuid":"b20aa5cb-45dd-43ce-8e7c-4e77244f644a"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 4","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 4 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146604","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t47","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146604,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146604,"related_publication":145873,"title":"Operator 4 inelastic isovector","uuid":"524e342a-2fc2-40d4-96ba-cf1a30fcefb1"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 7","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 7 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146605","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t48","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146605,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146605,"related_publication":145873,"title":"Operator 7 inelastic isovector","uuid":"37fbbf83-50b5-4fc1-8b50-0e6537d19b0c"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 9","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 9 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146606","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t49","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146606,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146606,"related_publication":145873,"title":"Operator 9 inelastic isovector","uuid":"2f590f92-0924-423c-9d2e-40ead4d9089b"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 3","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 3 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146607","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t50","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146607,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146607,"related_publication":145873,"title":"Operator 3 inelastic isovector","uuid":"0c2a46f2-3802-42e8-844d-59f0861206a8"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 11","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 11 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146608","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t51","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146608,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146608,"related_publication":145873,"title":"Operator 11 inelastic isovector","uuid":"3d209e57-6040-4e1c-98d5-5dc2e1b21258"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 5","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 5 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146609","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t52","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146609,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146609,"related_publication":145873,"title":"Operator 5 inelastic isovector","uuid":"c56fc7da-dd50-4cd5-8008-5664bae224d9"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 10","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 10 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146610","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t53","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146610,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146610,"related_publication":145873,"title":"Operator 10 inelastic isovector","uuid":"5e69c9ad-4332-4aee-af88-1bbed2696511"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 8","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 8 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146611","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t54","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146611,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146611,"related_publication":145873,"title":"Operator 8 inelastic isovector","uuid":"13fed142-4bd6-43b4-8a95-3dda20659125"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 14","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 14 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146612","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t55","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146612,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146612,"related_publication":145873,"title":"Operator 14 inelastic isovector","uuid":"2634049a-83d6-4e3d-8dc4-fa0e88da9c59"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 15","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 15 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146613","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t56","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146613,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146613,"related_publication":145873,"title":"Operator 15 inelastic isovector","uuid":"bbabb33b-a421-4b79-a9d2-b96739d77786"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 6","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 6 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146614","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t57","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146614,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146614,"related_publication":145873,"title":"Operator 6 inelastic isovector","uuid":"5a099639-c577-436f-a568-b202f8d439d5"},{"abstract":"Isovector WIMP-nucleon inelastic coupling limit for Operator 12","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isovector/csv","json":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isovector/json","root":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isovector/root","yaml":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isovector/yaml","yoda":"https://www.hepdata.net/download/table/ins2729878/Operator 12 inelastic isovector/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"146615","creation_date":"2023-12-04","data_keywords":{"cmenergies":[],"observables":["Operator coupling"]},"date":"04 Dec 2023","doc_type":"datatable","doi":"10.17182/hepdata.145873.v1/t58","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":146615,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"Operator coupling"}],"last_updated":"2024-01-17T12:28:24","parent_child_join":{"name":"child_datatable","parent":"145873"},"recid":146615,"related_publication":145873,"title":"Operator 12 inelastic isovector","uuid":"de695877-bb03-4e7b-a694-ac6d7221ae9a"}],"data_keywords":{"cmenergies":[],"observables":["Efficiency (%)","Operator coupling","S1c (phd)","log10(S2c) (phd)"]},"date":"04 Dec 2023","doc_type":"publication","doi":null,"first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"hepdata_doi":"10.17182/hepdata.145873","id":145873,"inspire_id":"2729878","journal_info":"No Journal Information","keywords":[{"schema":"INSPIRE","value":"dark matter: direct detection"},{"schema":"INSPIRE","value":"spin: dependence"},{"schema":"INSPIRE","value":"energy: upper limit"},{"schema":"INSPIRE","value":"time projection chamber: xenon"},{"schema":"INSPIRE","value":"xenon: liquid"},{"schema":"INSPIRE","value":"scintillation counter: liquid"},{"schema":"INSPIRE","value":"energy: high"},{"schema":"INSPIRE","value":"WIMP: dark matter"},{"schema":"INSPIRE","value":"WIMP nucleon: interaction"},{"schema":"INSPIRE","value":"effective field theory: nonrelativistic"},{"schema":"INSPIRE","value":"WIMP nucleon: scattering"},{"schema":"INSPIRE","value":"isoscalar"},{"schema":"INSPIRE","value":"isovector"},{"schema":"INSPIRE","value":"LUX"},{"schema":"INSPIRE","value":"ZEPLIN"},{"schema":"INSPIRE","value":"coupling constant: upper limit"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"}],"last_updated":"2024-01-17T12:28:32","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-03-22T00:00:00","recid":145873,"subject_area":["hep-ex","astro-ph.CO","Astrophysics"],"summary_authors":[{"affiliation":"SLAC","full_name":"Aalbers, J."},{"affiliation":"SLAC","full_name":"Akerib, D.S."},{"affiliation":"University Coll. London","full_name":"Musalhi, A.K. Al"},{"affiliation":"University Coll. London","full_name":"Alder, F."},{"affiliation":"Michigan U.","full_name":"Amarasinghe, C.S."},{"affiliation":"SLAC","full_name":"Ames, A."},{"affiliation":"SLAC","full_name":"Anderson, T.J."},{"affiliation":"Imperial Coll., London","full_name":"Angelides, N."},{"affiliation":"Imperial Coll., London","full_name":"Ara\u00fajo, H.M."},{"affiliation":"Maryland U.","full_name":"Armstrong, J.E."}],"title":"First Constraints on WIMP-Nucleon Effective Field Theory Couplings in an Extended Energy Region From LUX-ZEPLIN","total_tables":58,"type":["article"],"uuid":"a68ec3d4-9438-405a-aad6-6a20c879ffc8","version":1,"year":"2023"},{"abstract":"A search is reported for long-lived dark photons with masses between 0.1 GeV and 15 GeV, from exotic decays of Higgs bosons produced via vector-boson-fusion. Events that contain displaced collimated Standard Model fermions reconstructed in the calorimeter or muon spectrometer are probed. This search uses the full LHC Run 2 (2015-2018) data sample collected in proton-proton collisions at $\\sqrt{s}=13$ TeV, corresponding to an integrated luminosity of 139 $fb^{-1}$. Dominant backgrounds from Standard Model processes and non-collision sources are estimated by using data-driven techniques. The observed event yields in the signal regions are consistent with the expected background. Upper limits on the Higgs boson to dark photon branching fraction are reported as a function of the dark-photon mean proper decay length or of the dark-photon mass and the coupling between the Standard Model and the potential dark sector. This search is combined with previous ATLAS searches obtained in the gluon-gluon fusion and \\textit{WH} production modes. A branching fraction above 10% is excluded at 95% CL for a 125 GeV Higgs boson decaying into two dark photons for dark-photon mean proper decay lengths between 173 and 1296 mm and mass of 10 GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2728869/1/csv","json":"https://www.hepdata.net/download/submission/ins2728869/1/json","root":"https://www.hepdata.net/download/submission/ins2728869/1/root","yaml":"https://www.hepdata.net/download/submission/ins2728869/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2728869/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2311.18298","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"145164","creation_date":"2023-11-30","data":[{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for the SRμ search channel, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Figure 5a/csv","json":"https://www.hepdata.net/download/table/ins2728869/Figure 5a/json","root":"https://www.hepdata.net/download/table/ins2728869/Figure 5a/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Figure 5a/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Figure 5a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147235","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147235,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147235,"related_publication":145164,"title":"Figure 5a","uuid":"3235291d-8368-446a-9b92-b80290ed4286"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for the SRcL search channel, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Figure 5b/csv","json":"https://www.hepdata.net/download/table/ins2728869/Figure 5b/json","root":"https://www.hepdata.net/download/table/ins2728869/Figure 5b/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Figure 5b/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Figure 5b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147236","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147236,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147236,"related_publication":145164,"title":"Figure 5b","uuid":"86a8f0fc-2c10-420a-a210-ebc8c608dca7"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for the SRcH search channel, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Figure 5c/csv","json":"https://www.hepdata.net/download/table/ins2728869/Figure 5c/json","root":"https://www.hepdata.net/download/table/ins2728869/Figure 5c/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Figure 5c/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Figure 5c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147237","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147237,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147237,"related_publication":145164,"title":"Figure 5c","uuid":"d50e6082-06fb-426a-8447-b55237a0a70f"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for all search channels combined, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Figure 5d/csv","json":"https://www.hepdata.net/download/table/ins2728869/Figure 5d/json","root":"https://www.hepdata.net/download/table/ins2728869/Figure 5d/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Figure 5d/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Figure 5d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147238","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147238,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147238,"related_publication":145164,"title":"Figure 5d","uuid":"f0432392-f61a-4e87-932b-65a972c3d707"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for a γd mass of 100 MeV, as a function of the dark-photon mean proper decay length cτ. The solid black curve shows the observed exclusion limit from their statistical combination. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Figure 6a/csv","json":"https://www.hepdata.net/download/table/ins2728869/Figure 6a/json","root":"https://www.hepdata.net/download/table/ins2728869/Figure 6a/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Figure 6a/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Figure 6a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147239","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147239,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147239,"related_publication":145164,"title":"Figure 6a","uuid":"1c0744ca-a777-42b5-a5dc-61a0a7e7dd16"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for a γd mass of 10 GeV, as a function of the dark-photon mean proper decay length cτ. The solid black curve shows the observed exclusion limit from their statistical combination. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Figure 6b/csv","json":"https://www.hepdata.net/download/table/ins2728869/Figure 6b/json","root":"https://www.hepdata.net/download/table/ins2728869/Figure 6b/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Figure 6b/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Figure 6b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147240","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147240,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147240,"related_publication":145164,"title":"Figure 6b","uuid":"0215669d-8c2a-4967-9346-d86b095d1406"},{"abstract":"Acceptance times efficiency extrapolated as a function of cτγd for the μDPJ channel (SRμ), obtained for the different FRVZ MC signal mass points.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3a/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3a/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3a/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3a/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147241","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC/EFF"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147241,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"ACC/EFF"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147241,"related_publication":145164,"title":"Auxiliary figure 3a","uuid":"915a7b86-0bb3-47eb-a6ed-01e3de5e4322"},{"abstract":"Acceptance times efficiency extrapolated as a function of cτγd for the low ETmiss caloDPJ channel (SRcL), obtained for the different FRVZ MC signal mass points.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3b/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3b/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3b/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3b/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147242","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC/EFF"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147242,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"ACC/EFF"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147242,"related_publication":145164,"title":"Auxiliary figure 3b","uuid":"3d2be23f-0b76-4818-ae74-2cc602ff5796"},{"abstract":"Acceptance times efficiency extrapolated as a function of cτγd for the high ETmiss caloDPJ channel (SRcH), obtained for the different FRVZ MC signal mass points.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3c/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3c/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3c/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3c/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 3c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147243","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC/EFF"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147243,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"ACC/EFF"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147243,"related_publication":145164,"title":"Auxiliary figure 3c","uuid":"a796ca05-fd88-4126-a6f8-ecf0915d3a35"},{"abstract":"Observed (solid line) and expected (dashed line) 95% CL upper limits on B(H→ 2γd+X) for FRVZ processes with a 125 GeV Higgs boson as a function of dark photon mean proper decay length for the ggF, WH and VBF analyses. The full combination is shown as solid or dashed black lines for a dark photon mass of 17 MeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4a/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4a/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4a/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4a/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147244","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147244,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147244,"related_publication":145164,"title":"Auxiliary figure 4a","uuid":"e1c3d731-3bd1-486a-a652-fec03fb4a9be"},{"abstract":"Observed (solid line) and expected (dashed line) 95% CL upper limits on B(H→ 2γd+X) for FRVZ processes with a 125 GeV Higgs boson as a function of dark photon mean proper decay length for the ggF, WH and VBF analyses. The full combination is shown as solid or dashed black lines for a dark photon mass of 50 MeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4b/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4b/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4b/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4b/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147245","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147245,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147245,"related_publication":145164,"title":"Auxiliary figure 4b","uuid":"8a6934aa-8a1a-4e47-8ccc-9c24d247c297"},{"abstract":"Observed (solid line) and expected (dashed line) 95% CL upper limits on B(H→ 2γd+X) for FRVZ processes with a 125 GeV Higgs boson as a function of dark photon mean proper decay length for the ggF, WH and VBF analyses. The full combination is shown as solid or dashed black lines for a dark photon mass of 400 MeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4c/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4c/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4c/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4c/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147246","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147246,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147246,"related_publication":145164,"title":"Auxiliary figure 4c","uuid":"5d11c479-43dd-43d1-acfc-88ef47f7cf29"},{"abstract":"Observed (solid line) and expected (dashed line) 95% CL upper limits on B(H→ 2γd+X) for FRVZ processes with a 125 GeV Higgs boson as a function of dark photon mean proper decay length for the ggF, WH and VBF analyses. The full combination is shown as solid or dashed black lines for a dark photon mass of 900 MeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4d/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4d/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4d/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4d/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147247","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147247,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147247,"related_publication":145164,"title":"Auxiliary figure 4d","uuid":"434a39d2-cec6-4f50-9bf0-5c7f58186fd7"},{"abstract":"Observed (solid line) and expected (dashed line) 95% CL upper limits on B(H→ 2γd+X) for FRVZ processes with a 125 GeV Higgs boson as a function of dark photon mean proper decay length for the ggF, WH and VBF analyses. The full combination is shown as solid or dashed black lines for a dark photon mass of 2 GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4e/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4e/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4e/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4e/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4e/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147248","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147248,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147248,"related_publication":145164,"title":"Auxiliary figure 4e","uuid":"6aa087d0-90ea-404d-8268-7a1f2c06f786"},{"abstract":"Observed (solid line) and expected (dashed line) 95% CL upper limits on B(H→ 2γd+X) for FRVZ processes with a 125 GeV Higgs boson as a function of dark photon mean proper decay length for the ggF, WH and VBF analyses. The full combination is shown as solid or dashed black lines for a dark photon mass of 6 GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4f/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4f/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4f/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4f/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4f/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147249","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147249,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147249,"related_publication":145164,"title":"Auxiliary figure 4f","uuid":"58a588ab-547f-49e8-9a16-e703e3fd63be"},{"abstract":"Observed (solid line) and expected (dashed line) 95% CL upper limits on B(H→ 2γd+X) for FRVZ processes with a 125 GeV Higgs boson as a function of dark photon mean proper decay length for the ggF, WH and VBF analyses. The full combination is shown as solid or dashed black lines for a dark photon mass of 15 GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4g/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4g/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4g/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4g/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 4g/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147250","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147250,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147250,"related_publication":145164,"title":"Auxiliary figure 4g","uuid":"a2a97ff1-49fe-47a4-8389-28aa198c26ee"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for the SRμ search channel, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6a/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6a/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6a/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6a/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147251","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147251,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147251,"related_publication":145164,"title":"Auxiliary figure 6a","uuid":"6744f281-506d-4699-8301-060006b07ac2"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for the SRcL search channel, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6b/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6b/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6b/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6b/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147252","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147252,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147252,"related_publication":145164,"title":"Auxiliary figure 6b","uuid":"544f0189-06c6-4c16-8650-55befb79dbd3"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for the SRcH search channel, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6c/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6c/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6c/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6c/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147253","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t19","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147253,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147253,"related_publication":145164,"title":"Auxiliary figure 6c","uuid":"3ffc53b7-fbf4-4b9d-ae36-31f069831b91"},{"abstract":"Observed 95% CL upper limits on B(H→ 2γd+X) for different γd masses and a 125 GeV Higgs boson, as a function of the dark-photon mean proper decay length cτ. The limits are shown for all search channels combined, assuming an FRVZ signal model. The hatched band denotes the region in which the branching ratio is larger than unity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6d/csv","json":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6d/json","root":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6d/root","yaml":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6d/yaml","yoda":"https://www.hepdata.net/download/table/ins2728869/Auxiliary figure 6d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147254","creation_date":"2023-11-30","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145164.v1/t20","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147254,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Exotic Higgs decay"},{"name":"phrases","synonyms":"","value":"Long lived particles"},{"name":"phrases","synonyms":"","value":"Dark photon"},{"name":"reactions","synonyms":"","value":"P P --> 2γd+X"}],"last_updated":"2024-02-13T21:26:01","parent_child_join":{"name":"child_datatable","parent":"145164"},"recid":147254,"related_publication":145164,"title":"Auxiliary figure 6d","uuid":"63b42786-1b65-4e01-9148-4f837c5936b0"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ACC/EFF","CLS"],"phrases":["Dark photon","Long lived particles","Exotic Higgs decay"],"reactions":["P P --> 2γd+X"]},"date":"30 Nov 2023","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.145164","id":145164,"inspire_id":"2728869","journal_info":"CERN-EP-2023-226","keywords":[{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"decay: length"},{"schema":"INSPIRE","value":"Higgs particle: hadroproduction"},{"schema":"INSPIRE","value":"vector boson: fusion"},{"schema":"INSPIRE","value":"Higgs particle: rare decay"},{"schema":"INSPIRE","value":"Higgs particle: radiative decay"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"neutral particle: long-lived"},{"schema":"INSPIRE","value":"Higgs particle: branching ratio"},{"schema":"INSPIRE","value":"branching ratio: upper limit"},{"schema":"INSPIRE","value":"decay: exotic"},{"schema":"INSPIRE","value":"muon: spectrometer"},{"schema":"INSPIRE","value":"gluon gluon: fusion"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"background"},{"schema":"INSPIRE","value":"collimator"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"calorimeter"},{"schema":"INSPIRE","value":"photon: mass"},{"schema":"INSPIRE","value":"photon: pair production"},{"schema":"INSPIRE","value":"photon: hidden sector"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-02-13T21:26:04","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-02-13T00:00:00","recid":145164,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"},{"affiliation":"INFN, Udine","full_name":"Acharya, Bobby Samir"}],"title":"Search for light long-lived neutral particles from Higgs boson decays via vector-boson-fusion production from $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","total_tables":20,"type":["article"],"uuid":"047d100b-36f7-4728-86d9-c16da97deb77","version":1,"year":"2023"},{"abstract":"This paper reports cross-section measurements of $ZZ$ production in $pp$ collisions at $\\sqrt{s}=13.6$ TeV at the Large Hadron Collider. The data were collected by the ATLAS detector in 2022, and correspond to an integrated luminosity of 29 fb$^-1$. Events in the $ZZ\\rightarrow4\\ell$ ($\\ell = e$, $\\mu$) final states are selected and used to measure the inclusive and differential cross-sections in a fiducial region defined close to the analysis selections. The inclusive cross-section is further extrapolated to the total phase space with a requirement of 66 $< m_Z <$ 116 GeV for both $Z$ bosons, yielding $16.8 \\pm 1.1$ pb. The results are well described by the Standard Model predictions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2723369/1/csv","json":"https://www.hepdata.net/download/submission/ins2723369/1/json","root":"https://www.hepdata.net/download/submission/ins2723369/1/root","yaml":"https://www.hepdata.net/download/submission/ins2723369/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2723369/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2311.09715","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"144768","creation_date":"2023-11-16","data":[{"abstract":"The measured differential cross-sections compared to the predictions in the $m_{4\\ell}$ bins","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2723369/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2723369/Table 1/json","root":"https://www.hepdata.net/download/table/ins2723369/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2723369/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2723369/Table 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147067","creation_date":"2023-11-16","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0}],"observables":["XS"],"phrases":["ZZ Production"],"reactions":["P P --> Z Z --> 4l"]},"date":"16 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.144768.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147067,"inspire_id":"2723369","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"XS"},{"name":"reactions","synonyms":"","value":"P P --> Z Z --> 4l"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"ZZ Production"}],"last_updated":"2024-02-06T15:31:42","parent_child_join":{"name":"child_datatable","parent":"144768"},"recid":147067,"related_publication":144768,"title":"Table 1","uuid":"7e65b842-cdae-4aa8-95a5-55e082ba1415"},{"abstract":"The measured differential cross-sections compared to the predictions in the $p_T^{4\\ell}$ bins","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2723369/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2723369/Table 2/json","root":"https://www.hepdata.net/download/table/ins2723369/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2723369/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2723369/Table 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"147068","creation_date":"2023-11-16","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0}],"observables":["XS"],"phrases":["ZZ Production"],"reactions":["P P --> Z Z --> 4l"]},"date":"16 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.144768.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":147068,"inspire_id":"2723369","journal_info":"No Journal Information","keywords":[{"name":"observables","synonyms":"","value":"XS"},{"name":"reactions","synonyms":"","value":"P P --> Z Z --> 4l"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"ZZ Production"}],"last_updated":"2024-02-06T15:31:42","parent_child_join":{"name":"child_datatable","parent":"144768"},"recid":147068,"related_publication":144768,"title":"Table 2","uuid":"feadbce1-731c-4758-bf73-adb9ff4695c9"}],"data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0}],"observables":["XS"],"phrases":["ZZ Production"],"reactions":["P P --> Z Z --> 4l"]},"date":"16 Nov 2023","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.144768","id":144768,"inspire_id":"2723369","journal_info":"No Journal Information","keywords":[{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"Z0: pair production"},{"schema":"INSPIRE","value":"Z0: leptonic decay"},{"schema":"INSPIRE","value":"final state: (4lepton)"},{"schema":"INSPIRE","value":"mass spectrum: (4lepton)"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"differential cross section: measured"},{"schema":"INSPIRE","value":"mass dependence"},{"schema":"INSPIRE","value":"transverse momentum dependence"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"phase space"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13600 GeV-cms"}],"last_updated":"2024-02-06T15:31:42","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-02-06T00:00:00","recid":144768,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"},{"affiliation":"INFN, Udine","full_name":"Acharya, Bobby Samir"}],"title":"Measurement of $ZZ$ production cross-sections in the four-lepton final state in $pp$ collisions at $\\sqrt{s}=13.6$ TeV with the ATLAS experiment","total_tables":2,"type":["article"],"uuid":"0d58516f-df8a-43b5-991c-fdc6994f2ad7","version":1,"year":"2023"},{"abstract":"This paper presents a search for a new $Z^\\prime$ resonance decaying into a pair of dark quarks which hadronise into dark hadrons before promptly decaying back as Standard Model particles. This analysis is based on proton-proton collision data recorded at $\\sqrt{s}=13$ TeV with the ATLAS detector at the Large Hadron Collider between 2015 and 2018, corresponding to an integrated luminosity of 139 fb$^{-1}$. After selecting events containing large-radius jets with high track multiplicity, the invariant mass distribution of the two highest-transverse-momentum jets is scanned to look for an excess above a data-driven estimate of the Standard Model multijet background. No significant excess of events is observed and the results are thus used to set 95 % confidence-level upper limits on the production cross-section times branching ratio of the $Z^\\prime$ to dark quarks as a function of the $Z^\\prime$ mass for various dark-quark scenarios.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2719976/1/csv","json":"https://www.hepdata.net/download/submission/ins2719976/1/json","root":"https://www.hepdata.net/download/submission/ins2719976/1/root","yaml":"https://www.hepdata.net/download/submission/ins2719976/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2719976/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2311.03944","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"145191","creation_date":"2023-11-07","data":[{"abstract":"Distribution of the di-jet invariant mass, $m_{\\mathrm{JJ}}$ for the data, the simulated multi-jet background and of some representative signals (models A, B, C and D with $m_{Z'}=2.5$ TeV), shown after applying the preselections described in the text. The simulated background is normalised to the data and the signals are normalised to a production cross-section of 10 fb.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass after preselections/csv","json":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass after preselections/json","root":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass after preselections/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass after preselections/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass after preselections/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149494","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["M"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149494,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"M"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149494,"related_publication":145191,"title":"Di-jet invariant mass after preselections","uuid":"1c0f9c6a-7603-4e89-8e36-3c5bbd05d685"},{"abstract":"Distributions of the number of tracks associated to the leading jet, $n_{track,1}$, for the data, the simulated multi-jet background and of some representative signals (models A, B, C and D with $m_{Z^\\prime}=2.5$ TeV), shown after applying the preselections described in the text. All distributions are normalised to unity. The uncertainty band around the background prediction corresponds to the modelling uncertainty described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Leading jet number of tracks after preselections/csv","json":"https://www.hepdata.net/download/table/ins2719976/Leading jet number of tracks after preselections/json","root":"https://www.hepdata.net/download/table/ins2719976/Leading jet number of tracks after preselections/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Leading jet number of tracks after preselections/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Leading jet number of tracks after preselections/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149495","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149495,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149495,"related_publication":145191,"title":"Leading jet number of tracks after preselections","uuid":"6776d3a5-d5ec-4a02-86a9-74d2c9656eeb"},{"abstract":"Distributions of the number of tracks associated to the subleading jet, $n_{track,2}$, for the data, the simulated multi-jet background and of some representative signals (models A, B, C and D with $m_{Z^\\prime}=2.5$ TeV), shown after applying the preselections described in the text. All distributions are normalised to unity. The uncertainty band around the background prediction corresponds to the modelling uncertainty described in Section 6.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Sub-leading jet number of tracks after preselections/csv","json":"https://www.hepdata.net/download/table/ins2719976/Sub-leading jet number of tracks after preselections/json","root":"https://www.hepdata.net/download/table/ins2719976/Sub-leading jet number of tracks after preselections/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Sub-leading jet number of tracks after preselections/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Sub-leading jet number of tracks after preselections/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149496","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149496,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149496,"related_publication":145191,"title":"Sub-leading jet number of tracks after preselections","uuid":"3dcd2b39-42fc-444a-a591-bab3b77b5e34"},{"abstract":"Distribution of $m_{\\mathrm{JJ}}$ in the SR (black points) compared to the background-only expectation, where the shape is derived from the CR and the normalisation is fitted in the SR.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass in SR vs. background-only expectation/csv","json":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass in SR vs. background-only expectation/json","root":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass in SR vs. background-only expectation/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass in SR vs. background-only expectation/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Di-jet invariant mass in SR vs. background-only expectation/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149497","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["M"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149497,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"M"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149497,"related_publication":145191,"title":"Di-jet invariant mass in SR vs. background-only expectation","uuid":"1e97912f-c769-4523-b704-df10ab8b923e"},{"abstract":"Observed and expected limits at 95% CL on the cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model A (see the text for details). The darker and lighter shaded bands around the expected limits represent the $\\pm 1 \\sigma$ and $\\pm 2 \\sigma$ uncertainty range, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model A)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model A)/json","root":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model A)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model A)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model A)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149498","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149498,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149498,"related_publication":145191,"title":"Observed and expected limits (model A)","uuid":"52bb3ad6-9fe1-4dbc-9fc7-07bd718941cd"},{"abstract":"The predicted theory cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model A (see the text for details). In the theory model, a universal coupling of the $Z^\\prime$ to each SM quark $g_q$ is assumed and the dark quarks are all represented by one species with an effective coupling $g_{q_d}$ to the $Z^\\prime$. For model A, the predicted cross-section is shown for $g_q=0.05$ and $g_{q_d} = 0.2$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model A)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model A)/json","root":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model A)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model A)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model A)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149499","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149499,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149499,"related_publication":145191,"title":"Theory cross-section times branching ratio (model A)","uuid":"f782837c-7785-484e-8774-86b5f3aa232f"},{"abstract":"Observed and expected limits at 95% CL on the cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model B (see the text for details). The darker and lighter shaded bands around the expected limits represent the $\\pm 1 \\sigma$ and $\\pm 2 \\sigma$ uncertainty range, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model B)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model B)/json","root":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model B)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model B)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model B)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149500","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149500,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149500,"related_publication":145191,"title":"Observed and expected limits (model B)","uuid":"e23914ba-1ee9-48b4-aaba-6e0add7e3742"},{"abstract":"The predicted theory cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model B (see the text for details). In the theory model, a universal coupling of the $Z^\\prime$ to each SM quark $g_q$ is assumed and the dark quarks are all represented by one species with an effective coupling $g_{q_d}$ to the $Z^\\prime$. For model B, the predicted cross-section is shown for $g_q=0.15$ and $g_{q_d} = 0.5$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model B)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model B)/json","root":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model B)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model B)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model B)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149501","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149501,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149501,"related_publication":145191,"title":"Theory cross-section times branching ratio (model B)","uuid":"7c271331-6029-4a72-bdeb-5529c4be6ab0"},{"abstract":"Observed and expected limits at 95% CL on the cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model C (see the text for details). The darker and lighter shaded bands around the expected limits represent the $\\pm 1 \\sigma$ and $\\pm 2 \\sigma$ uncertainty range, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model C)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model C)/json","root":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model C)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model C)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model C)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149502","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149502,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149502,"related_publication":145191,"title":"Observed and expected limits (model C)","uuid":"f4b3b896-be7e-4344-98af-4e1ec43cb942"},{"abstract":"The predicted theory cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model C (see the text for details). In the theory model, a universal coupling of the $Z^\\prime$ to each SM quark $g_q$ is assumed and the dark quarks are all represented by one species with an effective coupling $g_{q_d}$ to the $Z^\\prime$. For model C, the predicted cross-section is shown for $g_q=0.15$ and $g_{q_d}= 0.5$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model C)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model C)/json","root":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model C)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model C)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model C)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149503","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149503,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149503,"related_publication":145191,"title":"Theory cross-section times branching ratio (model C)","uuid":"fe6a5477-0cca-4e05-af8f-e140b9a878a6"},{"abstract":"Observed and expected limits at 95% CL on the cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model D (see the text for details). The darker and lighter shaded bands around the expected limits represent the $\\pm 1 \\sigma$ and $\\pm 2 \\sigma$ uncertainty range, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model D)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model D)/json","root":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model D)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model D)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Observed and expected limits (model D)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149504","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149504,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"CLS"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149504,"related_publication":145191,"title":"Observed and expected limits (model D)","uuid":"c799495a-4959-4412-8b6c-1b855f04d9a7"},{"abstract":"The predicted theory cross-section times branching ratio for the production of dark quarks through a $Z^\\prime$ as a function of the $Z^\\prime$ mass for model D (see the text for details). In the theory model, a universal coupling of the $Z^\\prime$ to each SM quark $g_q$ is assumed and the dark quarks are all represented by one species with an effective coupling $g_{q_d}$ to the $Z^\\prime$. For model D, the predicted cross-section is shown for $g_q=0.05$ and $g_{q_d} = 0.2$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/json","root":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149505","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149505,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149505,"related_publication":145191,"title":"Theory cross-section times branching ratio (model D)","uuid":"fbf552b6-2257-48f4-9399-d25a5efae45f"},{"abstract":"Relative efficiency (in %) of each stage of the analysis selection with respect to the previous one for models A through D and $m_{Z^\\prime}=2.5$ TeV. Approximately 90000 events were generated per signal mass hypothesis.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/csv","json":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/json","root":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149506","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149506,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149506,"related_publication":145191,"title":"Cutflow table for signal points","uuid":"eec313ce-c239-4f90-82ab-0611cde4ec81"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS","M","EFF"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"publication","doi":"10.1007/JHEP02(2024)128","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.145191","id":145191,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"source":"author","value":"Beyond Standard Model"},{"source":"author","value":"Hadron-Hadron Scattering"},{"source":"author","value":"Dark Matter"},{"source":"author","value":"Exotics"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"jet: pair production"},{"schema":"INSPIRE","value":"resonance: production"},{"schema":"INSPIRE","value":"tracks: multiplicity"},{"schema":"INSPIRE","value":"multiplicity: high"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"jet: multiple production"},{"schema":"INSPIRE","value":"dijet: final state"},{"schema":"INSPIRE","value":"final state: ((n)jet)"},{"schema":"INSPIRE","value":"quark"},{"schema":"INSPIRE","value":"hidden sector"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"channel cross section: branching ratio: upper limit"},{"schema":"INSPIRE","value":"mass dependence"},{"schema":"INSPIRE","value":"Z': mass"},{"schema":"INSPIRE","value":"Z': hadronic decay"},{"schema":"INSPIRE","value":"dijet: mass spectrum"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"background"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-02-23T16:20:01","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-03-21T00:00:00","recid":145191,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"},{"affiliation":"INFN, Udine","full_name":"Acharya, Bobby Samir"}],"title":"Search for Resonant Production of Dark Quarks in the Dijet Final State with the ATLAS Detector","total_tables":13,"type":["article"],"uuid":"f232ecd8-3971-4045-98d2-fee1f5ff0918","version":1,"year":"2024"}],"total":5544}