{"facets":[{"max_values":5,"printable_name":"Observables","type":"observables","vals":[{"doc_count":164,"key":"SIG","url_params":{"observables":"SIG"}},{"doc_count":19,"key":"DSIG/DPT","url_params":{"observables":"DSIG/DPT"}},{"doc_count":18,"key":"SIG/SIG","url_params":{"observables":"SIG/SIG"}},{"doc_count":14,"key":"DSIG/DYRAP","url_params":{"observables":"DSIG/DYRAP"}},{"doc_count":13,"key":"N","url_params":{"observables":"N"}},{"doc_count":11,"key":"POL","url_params":{"observables":"POL"}},{"doc_count":10,"key":"DSIG/DT","url_params":{"observables":"DSIG/DT"}},{"doc_count":10,"key":"MULT","url_params":{"observables":"MULT"}},{"doc_count":9,"key":"ASYM","url_params":{"observables":"ASYM"}},{"doc_count":8,"key":"DSIG/DM","url_params":{"observables":"DSIG/DM"}}]},{"max_values":5,"printable_name":"Subject_areas","type":"subject_areas","vals":[{"doc_count":327,"key":"hep-ex","url_params":{"subject_areas":"hep-ex"}},{"doc_count":117,"key":"nucl-ex","url_params":{"subject_areas":"nucl-ex"}},{"doc_count":6,"key":"Phenomenology-HEP","url_params":{"subject_areas":"Phenomenology-HEP"}},{"doc_count":4,"key":"hep-ph","url_params":{"subject_areas":"hep-ph"}},{"doc_count":3,"key":"Astrophysics","url_params":{"subject_areas":"Astrophysics"}},{"doc_count":3,"key":"astro-ph.CO","url_params":{"subject_areas":"astro-ph.CO"}},{"doc_count":2,"key":"nucl-th","url_params":{"subject_areas":"nucl-th"}}]},{"max_values":5,"printable_name":"Collaboration","type":"collaboration","vals":[{"doc_count":167,"key":"CDF","url_params":{"collaboration":"CDF"}},{"doc_count":109,"key":"PHENIX","url_params":{"collaboration":"PHENIX"}},{"doc_count":28,"key":"L3","url_params":{"collaboration":"L3"}},{"doc_count":11,"key":"BESIII","url_params":{"collaboration":"BESIII"}},{"doc_count":11,"key":"D0","url_params":{"collaboration":"D0"}},{"doc_count":11,"key":"LHCB","url_params":{"collaboration":"LHCb"}},{"doc_count":8,"key":"LEPS","url_params":{"collaboration":"LEPS"}},{"doc_count":7,"key":"LHCF","url_params":{"collaboration":"LHCf"}},{"doc_count":6,"key":"CLEO","url_params":{"collaboration":"CLEO"}},{"doc_count":5,"key":"ATLAS","url_params":{"collaboration":"ATLAS"}}]},{"max_values":10,"printable_name":"Authors","type":"author","vals":[{"doc_count":205,"key":"Kim, D.H.","url_params":{"author":"Kim, D.H."}},{"doc_count":173,"key":"Kim, S.H.","url_params":{"author":"Kim, S.H."}},{"doc_count":172,"key":"Williams, H.H.","url_params":{"author":"Williams, H.H."}},{"doc_count":170,"key":"Franklin, M.","url_params":{"author":"Franklin, M."}},{"doc_count":169,"key":"Punzi, G.","url_params":{"author":"Punzi, G."}},{"doc_count":168,"key":"Barnes, V.E.","url_params":{"author":"Barnes, V.E."}},{"doc_count":168,"key":"Giannetti, P.","url_params":{"author":"Giannetti, P."}},{"doc_count":168,"key":"Kondo, K.","url_params":{"author":"Kondo, K."}},{"doc_count":168,"key":"Ristori, L.","url_params":{"author":"Ristori, L."}},{"doc_count":167,"key":"Apollinari, G.","url_params":{"author":"Apollinari, G."}}]},{"max_values":5,"printable_name":"Reactions","type":"reactions","vals":[{"doc_count":31,"key":"Au Au --> CHARGED X","url_params":{"reactions":"Au Au --> CHARGED X"}},{"doc_count":19,"key":"$p$ $p$ --> CHARGED X","url_params":{"reactions":"$p$ $p$ --> CHARGED X"}},{"doc_count":13,"key":"PBAR P --> W- X","url_params":{"reactions":"PBAR P --> W- X"}},{"doc_count":12,"key":"PBAR P --> W+ X","url_params":{"reactions":"PBAR P --> W+ X"}},{"doc_count":10,"key":"PBAR P --> Z0 X","url_params":{"reactions":"PBAR P --> Z0 X"}},{"doc_count":9,"key":"PBAR P --> TOP TOPBAR X","url_params":{"reactions":"PBAR P --> TOP TOPBAR X"}},{"doc_count":8,"key":"AU + AU --> CHARGED X0","url_params":{"reactions":"AU + AU --> CHARGED X0"}},{"doc_count":8,"key":"PBAR P --> JET X","url_params":{"reactions":"PBAR P --> JET X"}},{"doc_count":8,"key":"PBAR P --> MU+ MU- X","url_params":{"reactions":"PBAR P --> MU+ MU- X"}},{"doc_count":7,"key":"AU AU --> CHARGED X","url_params":{"reactions":"AU AU --> CHARGED X"}}]},{"max_values":5,"printable_name":"Date","type":"date","vals":[{"doc_count":29,"key":1997,"key_as_string":"1997-01-01T00:00:00.000Z","url_params":{"date":1997}},{"doc_count":23,"key":2010,"key_as_string":"2010-01-01T00:00:00.000Z","url_params":{"date":2010}},{"doc_count":22,"key":2005,"key_as_string":"2005-01-01T00:00:00.000Z","url_params":{"date":2005}},{"doc_count":21,"key":2001,"key_as_string":"2001-01-01T00:00:00.000Z","url_params":{"date":2001}},{"doc_count":19,"key":2002,"key_as_string":"2002-01-01T00:00:00.000Z","url_params":{"date":2002}},{"doc_count":19,"key":1998,"key_as_string":"1998-01-01T00:00:00.000Z","url_params":{"date":1998}},{"doc_count":18,"key":2007,"key_as_string":"2007-01-01T00:00:00.000Z","url_params":{"date":2007}},{"doc_count":17,"key":2008,"key_as_string":"2008-01-01T00:00:00.000Z","url_params":{"date":2008}},{"doc_count":17,"key":1996,"key_as_string":"1996-01-01T00:00:00.000Z","url_params":{"date":1996}},{"doc_count":16,"key":2009,"key_as_string":"2009-01-01T00:00:00.000Z","url_params":{"date":2009}},{"doc_count":15,"key":2006,"key_as_string":"2006-01-01T00:00:00.000Z","url_params":{"date":2006}},{"doc_count":15,"key":1994,"key_as_string":"1994-01-01T00:00:00.000Z","url_params":{"date":1994}},{"doc_count":15,"key":1993,"key_as_string":"1993-01-01T00:00:00.000Z","url_params":{"date":1993}},{"doc_count":14,"key":2012,"key_as_string":"2012-01-01T00:00:00.000Z","url_params":{"date":2012}},{"doc_count":14,"key":2011,"key_as_string":"2011-01-01T00:00:00.000Z","url_params":{"date":2011}},{"doc_count":14,"key":1995,"key_as_string":"1995-01-01T00:00:00.000Z","url_params":{"date":1995}},{"doc_count":12,"key":2015,"key_as_string":"2015-01-01T00:00:00.000Z","url_params":{"date":2015}},{"doc_count":11,"key":2004,"key_as_string":"2004-01-01T00:00:00.000Z","url_params":{"date":2004}},{"doc_count":11,"key":1990,"key_as_string":"1990-01-01T00:00:00.000Z","url_params":{"date":1990}},{"doc_count":9,"key":2023,"key_as_string":"2023-01-01T00:00:00.000Z","url_params":{"date":2023}},{"doc_count":9,"key":2013,"key_as_string":"2013-01-01T00:00:00.000Z","url_params":{"date":2013}},{"doc_count":9,"key":1992,"key_as_string":"1992-01-01T00:00:00.000Z","url_params":{"date":1992}},{"doc_count":9,"key":1989,"key_as_string":"1989-01-01T00:00:00.000Z","url_params":{"date":1989}},{"doc_count":8,"key":1991,"key_as_string":"1991-01-01T00:00:00.000Z","url_params":{"date":1991}},{"doc_count":7,"key":2014,"key_as_string":"2014-01-01T00:00:00.000Z","url_params":{"date":2014}},{"doc_count":7,"key":2003,"key_as_string":"2003-01-01T00:00:00.000Z","url_params":{"date":2003}},{"doc_count":7,"key":2000,"key_as_string":"2000-01-01T00:00:00.000Z","url_params":{"date":2000}},{"doc_count":6,"key":1981,"key_as_string":"1981-01-01T00:00:00.000Z","url_params":{"date":1981}},{"doc_count":5,"key":2016,"key_as_string":"2016-01-01T00:00:00.000Z","url_params":{"date":2016}},{"doc_count":5,"key":1982,"key_as_string":"1982-01-01T00:00:00.000Z","url_params":{"date":1982}},{"doc_count":4,"key":2022,"key_as_string":"2022-01-01T00:00:00.000Z","url_params":{"date":2022}},{"doc_count":4,"key":1988,"key_as_string":"1988-01-01T00:00:00.000Z","url_params":{"date":1988}},{"doc_count":4,"key":1980,"key_as_string":"1980-01-01T00:00:00.000Z","url_params":{"date":1980}},{"doc_count":3,"key":2018,"key_as_string":"2018-01-01T00:00:00.000Z","url_params":{"date":2018}},{"doc_count":3,"key":1999,"key_as_string":"1999-01-01T00:00:00.000Z","url_params":{"date":1999}},{"doc_count":3,"key":1983,"key_as_string":"1983-01-01T00:00:00.000Z","url_params":{"date":1983}},{"doc_count":3,"key":1972,"key_as_string":"1972-01-01T00:00:00.000Z","url_params":{"date":1972}},{"doc_count":2,"key":1978,"key_as_string":"1978-01-01T00:00:00.000Z","url_params":{"date":1978}},{"doc_count":2,"key":1971,"key_as_string":"1971-01-01T00:00:00.000Z","url_params":{"date":1971}},{"doc_count":2,"key":1969,"key_as_string":"1969-01-01T00:00:00.000Z","url_params":{"date":1969}},{"doc_count":2,"key":1968,"key_as_string":"1968-01-01T00:00:00.000Z","url_params":{"date":1968}},{"doc_count":1,"key":2021,"key_as_string":"2021-01-01T00:00:00.000Z","url_params":{"date":2021}},{"doc_count":1,"key":2020,"key_as_string":"2020-01-01T00:00:00.000Z","url_params":{"date":2020}},{"doc_count":1,"key":2019,"key_as_string":"2019-01-01T00:00:00.000Z","url_params":{"date":2019}},{"doc_count":1,"key":2017,"key_as_string":"2017-01-01T00:00:00.000Z","url_params":{"date":2017}},{"doc_count":1,"key":1977,"key_as_string":"1977-01-01T00:00:00.000Z","url_params":{"date":1977}},{"doc_count":1,"key":1975,"key_as_string":"1975-01-01T00:00:00.000Z","url_params":{"date":1975}},{"doc_count":1,"key":1974,"key_as_string":"1974-01-01T00:00:00.000Z","url_params":{"date":1974}},{"doc_count":1,"key":1966,"key_as_string":"1966-01-01T00:00:00.000Z","url_params":{"date":1966}},{"doc_count":1,"key":1965,"key_as_string":"1965-01-01T00:00:00.000Z","url_params":{"date":1965}},{"doc_count":0,"key":1987,"key_as_string":"1987-01-01T00:00:00.000Z","url_params":{"date":1987}},{"doc_count":0,"key":1986,"key_as_string":"1986-01-01T00:00:00.000Z","url_params":{"date":1986}},{"doc_count":0,"key":1985,"key_as_string":"1985-01-01T00:00:00.000Z","url_params":{"date":1985}},{"doc_count":0,"key":1984,"key_as_string":"1984-01-01T00:00:00.000Z","url_params":{"date":1984}},{"doc_count":0,"key":1979,"key_as_string":"1979-01-01T00:00:00.000Z","url_params":{"date":1979}},{"doc_count":0,"key":1976,"key_as_string":"1976-01-01T00:00:00.000Z","url_params":{"date":1976}},{"doc_count":0,"key":1973,"key_as_string":"1973-01-01T00:00:00.000Z","url_params":{"date":1973}},{"doc_count":0,"key":1970,"key_as_string":"1970-01-01T00:00:00.000Z","url_params":{"date":1970}},{"doc_count":0,"key":1967,"key_as_string":"1967-01-01T00:00:00.000Z","url_params":{"date":1967}}]},{"max_values":5,"printable_name":"Phrases","type":"phrases","vals":[{"doc_count":215,"key":"Inclusive","url_params":{"phrases":"Inclusive"}},{"doc_count":181,"key":"Cross Section","url_params":{"phrases":"Cross Section"}},{"doc_count":181,"key":"Integrated Cross Section","url_params":{"phrases":"Integrated Cross Section"}},{"doc_count":99,"key":"Exclusive","url_params":{"phrases":"Exclusive"}},{"doc_count":75,"key":"Single Differential Cross Section","url_params":{"phrases":"Single Differential Cross Section"}},{"doc_count":57,"key":"E+ E- Scattering","url_params":{"phrases":"E+ E- Scattering"}},{"doc_count":55,"key":"Muon production","url_params":{"phrases":"Muon production"}},{"doc_count":52,"key":"Electron production","url_params":{"phrases":"Electron production"}},{"doc_count":43,"key":"Jet Production","url_params":{"phrases":"Jet Production"}},{"doc_count":39,"key":"Transverse Momentum Dependence","url_params":{"phrases":"Transverse Momentum Dependence"}}]},{"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":444},"results":[{"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":"The LUX-ZEPLIN (LZ) experiment is a dark matter detector centered on a dual-phase xenon time projection chamber. We report searches for new physics appearing through few-keV-scale electron recoils, using the experiment's first exposure of 60 live days and a fiducial mass of 5.5t. The data are found to be consistent with a background-only hypothesis, and limits are set on models for new physics including solar axion electron coupling, solar neutrino magnetic moment and millicharge, and electron couplings to galactic axion-like particles and hidden photons. Similar limits are set on weakly interacting massive particle (WIMP) dark matter producing signals through ionized atomic states from the Migdal effect.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2683605/1/csv","json":"https://www.hepdata.net/download/submission/ins2683605/1/json","root":"https://www.hepdata.net/download/submission/ins2683605/1/root","yaml":"https://www.hepdata.net/download/submission/ins2683605/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2683605/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2307.15753","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":"144761","creation_date":"2023-07-28","data":[{"abstract":"The SR1 data in the {S1c, log10S2c} space with respect to observed time. Top plot is first half of SR1 containing 178 of the final data set. Bottom plot is second half of SR1 containing 157 events.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/LZ SR1 Data/csv","json":"https://www.hepdata.net/download/table/ins2683605/LZ SR1 Data/json","root":"https://www.hepdata.net/download/table/ins2683605/LZ SR1 Data/root","yaml":"https://www.hepdata.net/download/table/ins2683605/LZ SR1 Data/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/LZ SR1 Data/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145863","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["S1c (phd)","S2c (phd)","Time (days)"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t1","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145863,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"S1c (phd)"},{"name":"observables","synonyms":"","value":"S2c (phd)"},{"name":"observables","synonyms":"","value":"Time (days)"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145863,"related_publication":144761,"title":"LZ SR1 Data","uuid":"2ea5692b-7853-4466-ba80-46fa4c8b9e57"},{"abstract":"Electronic Recoil (ER) detection efficiency evaluated as a function of simulated true ER energy [keVee]. The data contains ER detection efficiency for ROI of study.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/Electronic Recoil Efficiency/csv","json":"https://www.hepdata.net/download/table/ins2683605/Electronic Recoil Efficiency/json","root":"https://www.hepdata.net/download/table/ins2683605/Electronic Recoil Efficiency/root","yaml":"https://www.hepdata.net/download/table/ins2683605/Electronic Recoil Efficiency/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/Electronic Recoil Efficiency/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145864","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["Efficiency (%)","Electronic Recoil Energy (keVee)"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t2","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145864,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"Electronic Recoil Energy (keVee)"},{"name":"observables","synonyms":"","value":"Efficiency (%)"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145864,"related_publication":144761,"title":"Electronic Recoil Efficiency","uuid":"0c03b851-408f-4184-9277-02a2af6c2c14"},{"abstract":"The observed 90% C.L upper limit on effective neutrino magnetic moment (\\mu_{\\nu}[\\mu_{B}]) in SR1. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Magnetic Moment/csv","json":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Magnetic Moment/json","root":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Magnetic Moment/root","yaml":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Magnetic Moment/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Magnetic Moment/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145865","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["Neutrino Magnetic Moment (\\mu_B)"],"reactions":["nu e -> nu e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t3","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145865,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"Neutrino Magnetic Moment (\\mu_B)"},{"name":"reactions","synonyms":"","value":"nu e -> nu e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145865,"related_publication":144761,"title":"Effective Neutrino Magnetic Moment","uuid":"6d4e0df5-0e8d-414a-8c3a-4e0b51ee6a3d"},{"abstract":"The observed 90% C.L upper limit on neutrino effective millicharge (\\delta_{Q}[e_{0}]) in SR1. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Milicharge/csv","json":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Milicharge/json","root":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Milicharge/root","yaml":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Milicharge/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/Effective Neutrino Milicharge/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145866","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["Neutrino Effective Milicharge e_0"],"reactions":["nu e -> nu e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t4","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145866,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"Neutrino Effective Milicharge e_0"},{"name":"reactions","synonyms":"","value":"nu e -> nu e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145866,"related_publication":144761,"title":"Effective Neutrino Milicharge","uuid":"e44ac894-80cb-436d-8d87-aedc8b71e74a"},{"abstract":"The observerd 90% C.L upper limit on solar axion g_{ae} coupling constant in valid across the mass range for SR1. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range as a function of Solar Axion Mass .","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/Solar Axion/csv","json":"https://www.hepdata.net/download/table/ins2683605/Solar Axion/json","root":"https://www.hepdata.net/download/table/ins2683605/Solar Axion/root","yaml":"https://www.hepdata.net/download/table/ins2683605/Solar Axion/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/Solar Axion/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145867","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["Solar Axion Mass (keV/c^2)","Axio-Electric Coupling (g_ae)"],"reactions":["a e -> a e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t5","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145867,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"Solar Axion Mass (keV/c^2)"},{"name":"observables","synonyms":"","value":"Axio-Electric Coupling (g_ae)"},{"name":"reactions","synonyms":"","value":"a e -> a e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145867,"related_publication":144761,"title":"Solar Axion","uuid":"6fe5df7d-885c-4e80-86c0-7aa24f1af111"},{"abstract":"The observed 90% C.L. upper limit on axion like particle (ALP) coupling constant (g_{ae}) in SR1. ALP mass spanning from 1 keV to 17 keV is considered. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range as a function of ALP Mass.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/Axion Like Particle (ALP)/csv","json":"https://www.hepdata.net/download/table/ins2683605/Axion Like Particle (ALP)/json","root":"https://www.hepdata.net/download/table/ins2683605/Axion Like Particle (ALP)/root","yaml":"https://www.hepdata.net/download/table/ins2683605/Axion Like Particle (ALP)/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/Axion Like Particle (ALP)/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145868","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["ALP Coupling Constant (g_ae)","ALP Mass (keV/c^2)"],"reactions":["a e -> a e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t6","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145868,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"ALP Mass (keV/c^2)"},{"name":"observables","synonyms":"","value":"ALP Coupling Constant (g_ae)"},{"name":"reactions","synonyms":"","value":"a e -> a e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145868,"related_publication":144761,"title":"Axion Like Particle (ALP)","uuid":"2b1c675c-3cea-43a3-8cba-57adcdba572a"},{"abstract":"The observed 90% C.L. upper limit on hidden photon (HP) coupling constant squared (\\kappa^2) in SR1. HP mass spanning from 1 keV to 17 keV is considered. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range as a function of HP Mass.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/Hidden Photon (HP)/csv","json":"https://www.hepdata.net/download/table/ins2683605/Hidden Photon (HP)/json","root":"https://www.hepdata.net/download/table/ins2683605/Hidden Photon (HP)/root","yaml":"https://www.hepdata.net/download/table/ins2683605/Hidden Photon (HP)/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/Hidden Photon (HP)/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145869","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["HP Mass (keV/c^2)","HP Coupling Constant (\\kappa^2)"],"reactions":["gamma e -> gamma e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t7","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145869,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"HP Mass (keV/c^2)"},{"name":"observables","synonyms":"","value":"HP Coupling Constant (\\kappa^2)"},{"name":"reactions","synonyms":"","value":"gamma e -> gamma e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145869,"related_publication":144761,"title":"Hidden Photon (HP)","uuid":"88dfdf6a-5740-4755-9d1c-779f3fceba0f"},{"abstract":"The observed 90% C.L. upper limit for the spin-independent (cm^2) WIMP cross-section vs. WIMP mass (GeV/c^2), using the Migdal signal pathway. The result is obtained for WIMPs undergoing the Migdal effect from 0.5 to 9 GeV/c2. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range as a function of WIMP Mass.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/SI WIMP cross-section/csv","json":"https://www.hepdata.net/download/table/ins2683605/SI WIMP cross-section/json","root":"https://www.hepdata.net/download/table/ins2683605/SI WIMP cross-section/root","yaml":"https://www.hepdata.net/download/table/ins2683605/SI WIMP cross-section/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/SI WIMP cross-section/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145870","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["Spin-Independent WIMP-nucleon Cross-section (cm^2)","WIMP Mass (GeV/c^2)"],"reactions":["chi e -> chi e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t8","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145870,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"WIMP Mass (GeV/c^2)"},{"name":"observables","synonyms":"","value":"Spin-Independent WIMP-nucleon Cross-section (cm^2)"},{"name":"reactions","synonyms":"","value":"chi e -> chi e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145870,"related_publication":144761,"title":"SI WIMP cross-section","uuid":"9eed9713-c48b-409f-8a4d-9335ca9400c2"},{"abstract":"The observed 90% C.L. upper limit for the spin-dependent WIMP cross-section (cm^2) vs. WIMP mass (GeV/c^2) for coupling on neutrons. The result is obtained for WIMPs undergoing the Migdal effect from 0.5 to 9 GeV/c2. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range as a function of WIMP Mass.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/SDn WIMP cross-section/csv","json":"https://www.hepdata.net/download/table/ins2683605/SDn WIMP cross-section/json","root":"https://www.hepdata.net/download/table/ins2683605/SDn WIMP cross-section/root","yaml":"https://www.hepdata.net/download/table/ins2683605/SDn WIMP cross-section/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/SDn WIMP cross-section/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145871","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["Spin-Dependent WIMP-neutron Cross-section (cm^2)","WIMP Mass (GeV/c^2)"],"reactions":["chi e -> chi e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t9","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145871,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"WIMP Mass (GeV/c^2)"},{"name":"observables","synonyms":"","value":"Spin-Dependent WIMP-neutron Cross-section (cm^2)"},{"name":"reactions","synonyms":"","value":"chi e -> chi e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145871,"related_publication":144761,"title":"SDn WIMP cross-section","uuid":"423a73ac-6a1f-4c1d-833e-9cb34753a37d"},{"abstract":"The observed 90% C.L. upper limit for the spin-dependent WIMP cross-section (cm^2) vs. WIMP mass (GeV/c^2) for coupling on protons. The result is obtained for WIMPs undergoing the Migdal effect from 0.5 to 9 GeV/c2. The data contains observed upper limit, median sensitivity and 1\\sigma and 2\\sigma sensitivity range as a function of WIMP Mass.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2683605/SDp WIMP cross-section/csv","json":"https://www.hepdata.net/download/table/ins2683605/SDp WIMP cross-section/json","root":"https://www.hepdata.net/download/table/ins2683605/SDp WIMP cross-section/root","yaml":"https://www.hepdata.net/download/table/ins2683605/SDp WIMP cross-section/yaml","yoda":"https://www.hepdata.net/download/table/ins2683605/SDp WIMP cross-section/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145872","creation_date":"2023-07-28","data_keywords":{"cmenergies":[],"observables":["Spin-Dependent WIMP-proton Cross-section (cm^2)","WIMP Mass (GeV/c^2)"],"reactions":["chi e -> chi e"]},"date":"28 Jul 2023","doc_type":"datatable","doi":"10.17182/hepdata.144761.v1/t10","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145872,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"name":"observables","synonyms":"","value":"WIMP Mass (GeV/c^2)"},{"name":"observables","synonyms":"","value":"Spin-Dependent WIMP-proton Cross-section (cm^2)"},{"name":"reactions","synonyms":"","value":"chi e -> chi e"}],"last_updated":"2023-12-11T14:29:36","parent_child_join":{"name":"child_datatable","parent":"144761"},"recid":145872,"related_publication":144761,"title":"SDp WIMP cross-section","uuid":"569cc9b8-6f35-42b4-85de-3f7ed71632dd"}],"data_keywords":{"cmenergies":[],"observables":["Solar Axion Mass (keV/c^2)","Axio-Electric Coupling (g_ae)","Electronic Recoil Energy (keVee)","ALP Mass (keV/c^2)","WIMP Mass (GeV/c^2)","Spin-Dependent WIMP-neutron Cross-section (cm^2)","Neutrino Magnetic Moment (\\mu_B)","HP Mass (keV/c^2)","Spin-Dependent WIMP-proton Cross-section (cm^2)","Time (days)","HP Coupling Constant (\\kappa^2)","S1c (phd)","ALP Coupling Constant (g_ae)","S2c (phd)","Efficiency (%)","Spin-Independent WIMP-nucleon Cross-section (cm^2)","Neutrino Effective Milicharge e_0"],"reactions":["nu e -> nu e","gamma e -> gamma e","a e -> a e","chi e -> chi e"]},"date":"28 Jul 2023","doc_type":"publication","doi":"10.1103/PhysRevD.108.072006","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"hepdata_doi":"10.17182/hepdata.144761","id":144761,"inspire_id":"2683605","journal_info":"Phys.Rev.D 108 (2023) 072006","keywords":[{"schema":"INSPIRE","value":"dark matter: direct detection"},{"schema":"INSPIRE","value":"dark matter: scattering"},{"schema":"INSPIRE","value":"electron: recoil"},{"schema":"INSPIRE","value":"new physics: search for"},{"schema":"INSPIRE","value":"coupling: (axion 2electron)"},{"schema":"INSPIRE","value":"time projection chamber: xenon"},{"schema":"INSPIRE","value":"photon: hidden sector"},{"schema":"INSPIRE","value":"axion: solar"},{"schema":"INSPIRE","value":"dark matter: detector"},{"schema":"INSPIRE","value":"neutrino: magnetic moment"},{"schema":"INSPIRE","value":"neutrino: solar"},{"schema":"INSPIRE","value":"WIMP: dark matter"},{"schema":"INSPIRE","value":"axion-like particles"},{"schema":"INSPIRE","value":"millicharge"},{"schema":"INSPIRE","value":"galaxy"},{"schema":"INSPIRE","value":"confidence limit"},{"schema":"INSPIRE","value":"coupling constant: upper limit"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"}],"last_updated":"2023-12-11T14:29:38","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-02-24T00:00:00","recid":144761,"subject_area":["Astrophysics","astro-ph.CO","hep-ex"],"summary_authors":[{"affiliation":"SLAC","full_name":"Aalbers, J."},{"affiliation":"SLAC","full_name":"Akerib, D.S."},{"affiliation":"Oxford U.","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":"A search for new physics in low-energy electron recoils from the first LZ exposure","total_tables":10,"type":["article"],"uuid":"7c98adc3-c5cb-4832-880e-1ddb4bc58bcd","version":1,"year":"2023"},{"abstract":"A precision measurement of the matrix elements for $\\eta\\to\\pi^+\\pi^-\\pi^0$ and $\\eta\\to\\pi^0\\pi^0\\pi^0$ decays is performed using a sample of $(10087\\pm44)\\times10^6$$J/\\psi$ decays collected with the BESIII detector. The decay $J/\\psi \\to \\gamma \\eta$ is used to select clean samples of 631,686 $\\eta\\to\\pi^+\\pi^-\\pi^0$ decays and 272,322 $\\eta\\to\\pi^0\\pi^0\\pi^0$ decays. The matrix elements for both channels are in reasonable agreement with previous measurements. The non-zero $gX^2Y$ term for the decay mode $\\eta\\to\\pi^+\\pi^-\\pi^0$ is confirmed, as reported by the KLOE Collaboration, while the other higher-order terms are found to be insignificant. Dalitz plot asymmetries in the $\\eta\\to\\pi^+\\pi^-\\pi^0$ decay are also explored and are found to be consistent with charge conjugation invariance. In addition, a cusp effect is investigated in the $\\eta\\to\\pi^0\\pi^0\\pi^0$ decay, and no obvious structure around the $\\pi^+\\pi^-$ mass threshold is observed.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2633025/1/csv","json":"https://www.hepdata.net/download/submission/ins2633025/1/json","root":"https://www.hepdata.net/download/submission/ins2633025/1/root","yaml":"https://www.hepdata.net/download/submission/ins2633025/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2633025/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2302.08282","authors":["Ablikim, M.","Achasov, M.N.","Adlarson, P.","Aliberti, R.","Amoroso, A.","An, M.R.","An, Q.","Bai, Y.","Bakina, O.","Balossino, I."],"collaborations":["BESIII"],"control_number":"141285","creation_date":"2023-02-16","data":[{"abstract":"The acceptance corrected $\\eta\\to\\pi^+\\pi^-\\pi^0$ data from 10 billion $J/\\psi$ events collected at BESIII and the corresponding statistical uncertainties in the Dalitz plot variables $X$ and $Y$. The data are divided into $20\\times20$ bins in $X$ and $Y$, and only the bins with non-zero event are listed in the table. The first two columns in the table are the center values of $X$ and $Y$, respectively. The last column is the acceptance corrected data and the corresponding statistical uncertainties.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_charge/csv","json":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_charge/json","root":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_charge/root","yaml":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_charge/yaml","yoda":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_charge/yoda"}},"authors":null,"collaborations":["BESIII"],"control_number":"141642","creation_date":"2023-02-16","data_keywords":{"cmenergies":[],"phrases":["Acceptance corrected data"],"reactions":["eta --> pi+ pi- pi0"]},"date":"16 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.141285.v1/t1","first_author":{"affiliation":"Beijing, Inst. High Energy Phys.","full_name":"Ablikim, M."},"id":141642,"inspire_id":"2633025","journal_info":"Phys.Rev.D 107 (2023) 092007","keywords":[{"name":"reactions","synonyms":"","value":"eta --> pi+ pi- pi0"},{"name":"phrases","synonyms":"","value":"Acceptance corrected data"}],"last_updated":"2023-07-09T08:46:06","parent_child_join":{"name":"child_datatable","parent":"141285"},"recid":141642,"related_publication":141285,"title":"DalitzPlot_eta23pi_charge","uuid":"ed293a43-3186-4fce-b16a-c3e1177b3b16"},{"abstract":"The acceptance corrected $\\eta\\to\\pi^0\\pi^0\\pi^0$ data from 10 billion $J/\\psi$ events collected at BESIII and the corresponding statistical uncertainties in the Dalitz plot variables $X$ and $Y$. The data are divided into $20\\times20$ bins in $X$ and $Y$, and only the bins with non-zero event are listed in the table. The first two columns in the table are the center values of $X$ and $Y$, respectively. The last column is the acceptance corrected data and the corresponding statistical uncertainties.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_neutral/csv","json":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_neutral/json","root":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_neutral/root","yaml":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_neutral/yaml","yoda":"https://www.hepdata.net/download/table/ins2633025/DalitzPlot_eta23pi_neutral/yoda"}},"authors":null,"collaborations":["BESIII"],"control_number":"141643","creation_date":"2023-02-16","data_keywords":{"cmenergies":[],"phrases":["Acceptance corrected data"],"reactions":["eta --> pi0 pi0 pi0"]},"date":"16 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.141285.v1/t2","first_author":{"affiliation":"Beijing, Inst. High Energy Phys.","full_name":"Ablikim, M."},"id":141643,"inspire_id":"2633025","journal_info":"Phys.Rev.D 107 (2023) 092007","keywords":[{"name":"reactions","synonyms":"","value":"eta --> pi0 pi0 pi0"},{"name":"phrases","synonyms":"","value":"Acceptance corrected data"}],"last_updated":"2023-07-09T08:46:06","parent_child_join":{"name":"child_datatable","parent":"141285"},"recid":141643,"related_publication":141285,"title":"DalitzPlot_eta23pi_neutral","uuid":"f83321be-7812-4464-807c-8be14712688b"}],"data_keywords":{"cmenergies":[],"phrases":["Acceptance corrected data"],"reactions":["eta --> pi+ pi- pi0","eta --> pi0 pi0 pi0"]},"date":"16 Feb 2023","doc_type":"publication","doi":"10.1103/PhysRevD.107.092007","first_author":{"affiliation":"Beijing, Inst. High Energy Phys.","full_name":"Ablikim, M."},"hepdata_doi":"10.17182/hepdata.141285","id":141285,"inspire_id":"2633025","journal_info":"Phys.Rev.D 107 (2023) 092007","keywords":[{"schema":"INSPIRE","value":"electron positron: annihilation"},{"schema":"INSPIRE","value":"electron positron: colliding beams"},{"schema":"INSPIRE","value":"J/psi(3100): electroproduction"},{"schema":"INSPIRE","value":"J/psi(3100): radiative decay"},{"schema":"INSPIRE","value":"eta: hadronic decay"},{"schema":"INSPIRE","value":"mass: threshold"},{"schema":"INSPIRE","value":"charge conjugation: invariance"},{"schema":"INSPIRE","value":"precision measurement"},{"schema":"INSPIRE","value":"eta: decay modes"},{"schema":"INSPIRE","value":"higher-order"},{"schema":"INSPIRE","value":"cusp effect"},{"schema":"INSPIRE","value":"asymmetry"},{"schema":"INSPIRE","value":"KLOE"},{"schema":"INSPIRE","value":"Dalitz plot"},{"schema":"INSPIRE","value":"mass spectrum: (pi+ pi-)"},{"schema":"INSPIRE","value":"BES"},{"schema":"INSPIRE","value":"structure"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"J/psi(3100) --> photon eta"},{"schema":"INSPIRE","value":"eta --> pi+ pi- pi0"},{"schema":"INSPIRE","value":"eta --> 3pi0"}],"last_updated":"2023-07-09T08:46:06","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-11T00:00:00","recid":141285,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Beijing, Inst. High Energy Phys.","full_name":"Ablikim, M."},{"affiliation":"Novosibirsk, IYF","full_name":"Achasov, M.N."},{"affiliation":"Uppsala U.","full_name":"Adlarson, P."},{"affiliation":"Mainz U., Inst. Phys.","full_name":"Aliberti, R."},{"affiliation":"INFN, Turin","full_name":"Amoroso, A."},{"affiliation":"Liaoning Normal U.","full_name":"An, M.R."},{"affiliation":"Hefei, NSRL","full_name":"An, Q."},{"affiliation":"Southeast U., Nanjing","full_name":"Bai, Y."},{"affiliation":"Dubna, JINR","full_name":"Bakina, O."},{"affiliation":"INFN, Ferrara","full_name":"Balossino, I."}],"title":"Precision measurement of the matrix elements for $\\eta\\to\\pi^+\\pi^-\\pi^0$ and $\\eta\\to\\pi^0\\pi^0\\pi^0$ decays","total_tables":2,"type":["article"],"uuid":"e5974456-85d9-4e94-b12b-8482d3e8894f","version":1,"year":"2023"},{"abstract":"Measurements of the suppression and correlations of dijets is performed using 3 $\\mu$b$^{-1}$ of Xe+Xe data at $\\sqrt{s_{\\mathrm{NN}}} = 5.44$ TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\\text{T}}$ over the range of 32 GeV to 398 GeV and the centrality of the collisions. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\\text{T}}$ balance are compared with previous Pb+Pb measurements at $\\sqrt{s_{\\mathrm{NN}}} =5.02$ TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear-modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference between the center-of-mass energies of the initial parton scattering process in Xe+Xe and Pb+Pb collisions. These results should provide input for a better understanding of the role of energy density, system size, path length, and fluctuations in the parton energy loss.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2630510/1/csv","json":"https://www.hepdata.net/download/submission/ins2630510/1/json","root":"https://www.hepdata.net/download/submission/ins2630510/1/root","yaml":"https://www.hepdata.net/download/submission/ins2630510/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2630510/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2302.03967","authors":["Aad, G.","Abbott, B.","Abeling, K.","Abidi, S.H.","Aboulhorma, A.","Abramowicz, H.","Abreu, H.","Abulaiti, Y.","Abusleme Hoffman, A.C.","Acharya, B.S."],"collaborations":["ATLAS"],"control_number":"139684","creation_date":"2023-02-08","data":[{"abstract":"The centrality intervals in Xe+Xe collisions and their corresponding TAA with absolute uncertainties.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2630510/Table 1/json","root":"https://www.hepdata.net/download/table/ins2630510/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Table 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141750","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["XE XE --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t1","first_author":{},"id":141750,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"XE XE --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141750,"related_publication":139684,"title":"Table 1","uuid":"55ac43b9-9aad-42bb-8954-d626ce1de0ac"},{"abstract":"The centrality intervals in Xe+Xe and Pb+Pb collisions for matching SUM ET FCAL intervals and respective TAA values for Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2630510/Table 2/json","root":"https://www.hepdata.net/download/table/ins2630510/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Table 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141751","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["XE XE --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t2","first_author":{},"id":141751,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"XE XE --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141751,"related_publication":139684,"title":"Table 2","uuid":"f037d2f1-a323-4a67-91f3-150a0f7cab02"},{"abstract":"The performance of the jet energy scale (JES) for jets with $|y| < 2.1$ evaluated as a function of pT_truth in different centrality bins. Simulated hard scatter events were overlaid onto events from a dedicated sample of minimum-bias Xe+Xe data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 1a/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 1a/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 1a/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 1a/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 1a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141752","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t3","first_author":{},"id":141752,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141752,"related_publication":139684,"title":"Figure 1a","uuid":"e32b4a69-72bf-4364-afdd-7597def1254c"},{"abstract":"The performance of jet energy resolution (JER) for jets with |y| < 2.1 evaluated as a function of pT_truth in different centrality bins. Simulated hard scatter events were overlaid onto events from a dedicated sample of minimum-bias Xe+Xe data. The fit parameters are listed in a sperate table (Extras 1)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 1b/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 1b/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 1b/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 1b/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 1b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141753","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t4","first_author":{},"id":141753,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141753,"related_publication":139684,"title":"Figure 1b","uuid":"e33cca19-5138-4208-9df4-a8251c26b7a9"},{"abstract":"The relative magnitude of systematic uncertainties for per-pair normalized xJ distributions in 0-10% Xe+Xe centrality","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 2a/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 2a/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 2a/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 2a/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 2a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141754","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t5","first_author":{},"id":141754,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141754,"related_publication":139684,"title":"Figure 2a","uuid":"eccdd590-b743-4403-a10a-9a0c591bf63e"},{"abstract":"The relative magnitude of systematic uncertainties for absolutely normalized xJ distributions in 0-10% Xe+Xe centrality","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 2b/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 2b/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 2b/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 2b/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 2b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141755","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t6","first_author":{},"id":141755,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141755,"related_publication":139684,"title":"Figure 2b","uuid":"9f83653b-10bc-4a2e-8b67-b2dfe01e0c16"},{"abstract":"The relative magnitude of systematic uncertainties for rho distributions for leading jets in 0-10% Xe+Xe centrality","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 2c/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 2c/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 2c/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 2c/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 2c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141756","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t7","first_author":{},"id":141756,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141756,"related_publication":139684,"title":"Figure 2c","uuid":"531ef2a4-3d89-41d0-bc49-0530ebc00295"},{"abstract":"Per-pair normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 3a/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 3a/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 3a/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 3a/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 3a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141757","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t8","first_author":{},"id":141757,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141757,"related_publication":139684,"title":"Figure 3a","uuid":"c8722d1a-a7af-4c98-b8cd-7a31e1c822c7"},{"abstract":"Per-pair normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 3b/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 3b/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 3b/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 3b/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 3b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141758","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t9","first_author":{},"id":141758,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141758,"related_publication":139684,"title":"Figure 3b","uuid":"b7fa3caa-f2b6-4fe4-8c52-d0860df110e7"},{"abstract":"Per-pair normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 3c/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 3c/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 3c/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 3c/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 3c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141759","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t10","first_author":{},"id":141759,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141759,"related_publication":139684,"title":"Figure 3c","uuid":"2fa43ca2-56ae-4144-8fa1-f45e2a1f9532"},{"abstract":"Absolutely normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 4a/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 4a/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 4a/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 4a/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 4a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141760","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t11","first_author":{},"id":141760,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141760,"related_publication":139684,"title":"Figure 4a","uuid":"69815ffd-794b-408d-8d87-900309718e77"},{"abstract":"Absolutely normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 4b/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 4b/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 4b/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 4b/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 4b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141761","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t12","first_author":{},"id":141761,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141761,"related_publication":139684,"title":"Figure 4b","uuid":"49dd1fd9-bdde-438a-ae22-5df9faa5d878"},{"abstract":"Absolutely normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 4c/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 4c/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 4c/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 4c/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 4c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141762","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t13","first_author":{},"id":141762,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141762,"related_publication":139684,"title":"Figure 4c","uuid":"0bdb7988-9f36-47b2-ade7-ed7c2e530d45"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 5a XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 5a XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 5a XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 5a XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 5a XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141763","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t14","first_author":{},"id":141763,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141763,"related_publication":139684,"title":"Figure 5a XeXe","uuid":"5221c37d-5a72-4252-8c7a-b7474ee331c8"},{"abstract":"Per-pair normalized xJ distribution in Pb+Pb collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 5a PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 5a PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 5a PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 5a PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 5a PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141764","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t15","first_author":{},"id":141764,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141764,"related_publication":139684,"title":"Figure 5a PbPb","uuid":"dcabcee3-7faf-4450-bcbc-3bb22fadfd78"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 5b XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 5b XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 5b XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 5b XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 5b XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141765","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t16","first_author":{},"id":141765,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141765,"related_publication":139684,"title":"Figure 5b XeXe","uuid":"32129db4-5489-48fc-9d15-4e5146b4772e"},{"abstract":"Per-pair normalized xJ distribution in Pb+Pb collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 5b PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 5b PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 5b PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 5b PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 5b PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141766","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t17","first_author":{},"id":141766,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141766,"related_publication":139684,"title":"Figure 5b PbPb","uuid":"f7e7d9ee-8d7b-4999-babd-a2cdb7e77b6c"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 5c XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 5c XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 5c XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 5c XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 5c XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141767","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t18","first_author":{},"id":141767,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141767,"related_publication":139684,"title":"Figure 5c XeXe","uuid":"5da21e7b-05ed-43c4-8eb2-3f9fab16a212"},{"abstract":"Per-pair normalized xJ distribution in Pb+Pb collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 5c PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 5c PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 5c PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 5c PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 5c PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141768","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t19","first_author":{},"id":141768,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141768,"related_publication":139684,"title":"Figure 5c PbPb","uuid":"a9aad231-ba58-4599-ae0a-b532d1b196d1"},{"abstract":"Absolutely normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6a XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6a XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6a XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6a XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6a XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141769","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t20","first_author":{},"id":141769,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141769,"related_publication":139684,"title":"Figure 6a XeXe","uuid":"76abd4f7-87d1-4537-8a88-e623f7a8ecbc"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6a PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6a PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6a PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6a PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6a PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141770","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t21","first_author":{},"id":141770,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141770,"related_publication":139684,"title":"Figure 6a PbPb","uuid":"d8c17b8e-1718-4a93-90af-4787db7a6db5"},{"abstract":"Absolutely normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6b XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6b XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6b XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6b XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6b XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141771","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t22","first_author":{},"id":141771,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141771,"related_publication":139684,"title":"Figure 6b XeXe","uuid":"f7c8aed0-8bc8-4543-9f12-3035d27e74e1"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6b PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6b PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6b PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6b PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6b PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141772","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t23","first_author":{},"id":141772,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141772,"related_publication":139684,"title":"Figure 6b PbPb","uuid":"9c720aa7-0d88-4b5e-83ae-598d460ebb77"},{"abstract":"Absolutely normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6c XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6c XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6c XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6c XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6c XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141773","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t24","first_author":{},"id":141773,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141773,"related_publication":139684,"title":"Figure 6c XeXe","uuid":"82a83fc4-fdb5-4007-afbd-4161de6e2974"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6c PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6c PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6c PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6c PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6c PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141774","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t25","first_author":{},"id":141774,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141774,"related_publication":139684,"title":"Figure 6c PbPb","uuid":"8659b7fd-4156-4c3d-a1e6-5b2f815ab78c"},{"abstract":"Absolutely normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6d XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6d XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6d XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6d XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6d XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141775","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t26","first_author":{},"id":141775,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141775,"related_publication":139684,"title":"Figure 6d XeXe","uuid":"54ddc7b5-cafa-466b-b28f-d341ab27e768"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6d PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6d PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6d PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6d PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6d PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141776","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t27","first_author":{},"id":141776,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141776,"related_publication":139684,"title":"Figure 6d PbPb","uuid":"6f3893d8-9f4b-4679-8d55-486685a65d74"},{"abstract":"Absolutely normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6e XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6e XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6e XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6e XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6e XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141777","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t28","first_author":{},"id":141777,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141777,"related_publication":139684,"title":"Figure 6e XeXe","uuid":"f111370b-3608-43cc-997e-865b9a2098bc"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6e PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6e PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6e PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6e PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6e PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141778","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t29","first_author":{},"id":141778,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141778,"related_publication":139684,"title":"Figure 6e PbPb","uuid":"9e7c1d4a-9eaa-4626-8f82-303ad7926f1e"},{"abstract":"Absolutely normalized xJ distribution in Xe+Xe collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6f XeXe/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6f XeXe/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6f XeXe/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6f XeXe/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6f XeXe/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141779","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t30","first_author":{},"id":141779,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141779,"related_publication":139684,"title":"Figure 6f XeXe","uuid":"a56760fe-c665-4c35-933a-2d4c850cb4d3"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 6f PbPb/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 6f PbPb/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 6f PbPb/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 6f PbPb/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 6f PbPb/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141780","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t31","first_author":{},"id":141780,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141780,"related_publication":139684,"title":"Figure 6f PbPb","uuid":"0f7ab150-54c2-4069-a5de-4abe301e83ea"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of leading jet pT in the same centrality intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 7a/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 7a/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 7a/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 7a/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 7a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141781","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t32","first_author":{},"id":141781,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141781,"related_publication":139684,"title":"Figure 7a","uuid":"826a7d18-899f-45cf-9c39-35414acd75fc"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of leading jet pT in the same centrality intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 7b/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 7b/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 7b/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 7b/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 7b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141782","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t33","first_author":{},"id":141782,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141782,"related_publication":139684,"title":"Figure 7b","uuid":"9b4de43d-9ed7-41f0-acdd-5cf5e2ab1dac"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of leading jet pT in the same centrality intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 7c/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 7c/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 7c/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 7c/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 7c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141783","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t34","first_author":{},"id":141783,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141783,"related_publication":139684,"title":"Figure 7c","uuid":"4446ae32-b1fa-4a1b-981c-1986b003b99c"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of subleading jet pT in the same centrality intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 7d/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 7d/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 7d/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 7d/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 7d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141784","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t35","first_author":{},"id":141784,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141784,"related_publication":139684,"title":"Figure 7d","uuid":"3112facd-e11c-4830-a64f-5f28e9a8a70c"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of subleading jet pT in the same centrality intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 7e/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 7e/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 7e/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 7e/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 7e/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141785","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t36","first_author":{},"id":141785,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141785,"related_publication":139684,"title":"Figure 7e","uuid":"efc2b907-d3c3-4aba-972e-d25b7f803165"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of subleading jet pT in the same centrality intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 7f/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 7f/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 7f/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 7f/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 7f/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141786","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t37","first_author":{},"id":141786,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141786,"related_publication":139684,"title":"Figure 7f","uuid":"53c02ae5-cd28-40e3-b8ca-c5b60472f1f7"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of leading jet pT in the same SUM ETFCal intervals (selecting equivalent event activity)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 8a/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 8a/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 8a/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 8a/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 8a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141787","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t38","first_author":{},"id":141787,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141787,"related_publication":139684,"title":"Figure 8a","uuid":"60ac2c8f-f039-4cd3-a807-3283e6acad3b"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of leading jet pT in the same SUM ETFCal intervals (selecting equivalent event activity)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 8b/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 8b/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 8b/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 8b/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 8b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141788","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t39","first_author":{},"id":141788,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141788,"related_publication":139684,"title":"Figure 8b","uuid":"86796456-f722-436e-8ee2-c15381686a65"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of leading jet pT in the same SUM ETFCal intervals (selecting equivalent event activity)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 8c/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 8c/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 8c/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 8c/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 8c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141789","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t40","first_author":{},"id":141789,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141789,"related_publication":139684,"title":"Figure 8c","uuid":"15110b97-8812-455e-9f87-67c2869a5c53"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of subleading jet pT in the same SUM ETFCal intervals (selecting equivalent event activity)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 8d/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 8d/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 8d/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 8d/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 8d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141790","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t41","first_author":{},"id":141790,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141790,"related_publication":139684,"title":"Figure 8d","uuid":"6ee8aadb-fad7-4d8c-b2b6-8ac920c55b25"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of subleading jet pT in the same SUM ETFCal intervals (selecting equivalent event activity)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 8e/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 8e/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 8e/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 8e/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 8e/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141791","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t42","first_author":{},"id":141791,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141791,"related_publication":139684,"title":"Figure 8e","uuid":"e6060c14-cb5b-4b19-871e-ff92bbb512af"},{"abstract":"The ratios of Xe+Xe and Pb+Pb pair nuclear-modification factors, rho, evaluated as a function of subleading jet pT in the same SUM ETFCal intervals (selecting equivalent event activity)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 8f/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 8f/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 8f/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 8f/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 8f/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141792","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["PB PB --> JETS X"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t43","first_author":{},"id":141792,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> JETS X"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141792,"related_publication":139684,"title":"Figure 8f","uuid":"4fc6a932-7483-45fb-9175-52ed794194f0"},{"abstract":"Parameter a,b, and c from JER fits in Figure 1b.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/JER Fit Parameters/csv","json":"https://www.hepdata.net/download/table/ins2630510/JER Fit Parameters/json","root":"https://www.hepdata.net/download/table/ins2630510/JER Fit Parameters/root","yaml":"https://www.hepdata.net/download/table/ins2630510/JER Fit Parameters/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/JER Fit Parameters/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141793","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["XE XE --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t44","first_author":{},"id":141793,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"XE XE --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141793,"related_publication":139684,"title":"JER Fit Parameters","uuid":"97eb517d-a14d-4234-b004-1c71e964f9bc"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10a XeXe 100-126 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10a XeXe 100-126 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10a XeXe 100-126 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10a XeXe 100-126 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10a XeXe 100-126 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141794","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t45","first_author":{},"id":141794,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141794,"related_publication":139684,"title":"Figure 10a XeXe 100-126 GeV","uuid":"15b02bc4-945b-4380-bc46-191985ac450b"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10a PbPb 100-126 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10a PbPb 100-126 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10a PbPb 100-126 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10a PbPb 100-126 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10a PbPb 100-126 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141795","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t46","first_author":{},"id":141795,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141795,"related_publication":139684,"title":"Figure 10a PbPb 100-126 GeV","uuid":"42433b45-5d7a-4670-8cac-c0b575db451b"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10b XeXe 100-126 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10b XeXe 100-126 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10b XeXe 100-126 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10b XeXe 100-126 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10b XeXe 100-126 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141796","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t47","first_author":{},"id":141796,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141796,"related_publication":139684,"title":"Figure 10b XeXe 100-126 GeV","uuid":"da7cb0b3-438e-46f8-8d19-6ea8b7aaeb0f"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10b PbPb 100-126 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10b PbPb 100-126 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10b PbPb 100-126 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10b PbPb 100-126 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10b PbPb 100-126 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141797","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t48","first_author":{},"id":141797,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141797,"related_publication":139684,"title":"Figure 10b PbPb 100-126 GeV","uuid":"3f9c8645-5d08-49ce-8aaa-f33bbfea5586"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10c XeXe 100-126 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10c XeXe 100-126 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10c XeXe 100-126 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10c XeXe 100-126 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10c XeXe 100-126 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141798","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t49","first_author":{},"id":141798,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141798,"related_publication":139684,"title":"Figure 10c XeXe 100-126 GeV","uuid":"bb5eeada-4036-446e-9f30-7876b48d47bb"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10c PbPb 100-126 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10c PbPb 100-126 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10c PbPb 100-126 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10c PbPb 100-126 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10c PbPb 100-126 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141799","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t50","first_author":{},"id":141799,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141799,"related_publication":139684,"title":"Figure 10c PbPb 100-126 GeV","uuid":"cac58949-ba15-4f15-aca9-eb0155e890f2"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10d XeXe 126-158 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10d XeXe 126-158 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10d XeXe 126-158 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10d XeXe 126-158 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10d XeXe 126-158 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141800","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t51","first_author":{},"id":141800,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141800,"related_publication":139684,"title":"Figure 10d XeXe 126-158 GeV","uuid":"7f72f815-a88a-468c-b306-a506f2585b26"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10d PbPb 126-158 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10d PbPb 126-158 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10d PbPb 126-158 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10d PbPb 126-158 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10d PbPb 126-158 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141801","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t52","first_author":{},"id":141801,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141801,"related_publication":139684,"title":"Figure 10d PbPb 126-158 GeV","uuid":"d80a2485-7ac6-4d27-9691-ebf2b361f440"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10e XeXe 126-158 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10e XeXe 126-158 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10e XeXe 126-158 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10e XeXe 126-158 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10e XeXe 126-158 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141802","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t53","first_author":{},"id":141802,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141802,"related_publication":139684,"title":"Figure 10e XeXe 126-158 GeV","uuid":"169a7ee6-10fa-414a-a76e-d54205eda5e0"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10e PbPb 126-158 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10e PbPb 126-158 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10e PbPb 126-158 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10e PbPb 126-158 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10e PbPb 126-158 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141803","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t54","first_author":{},"id":141803,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141803,"related_publication":139684,"title":"Figure 10e PbPb 126-158 GeV","uuid":"ce54b317-7096-4f65-a83f-5ab18139c07e"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10f XeXe 126-158 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10f XeXe 126-158 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10f XeXe 126-158 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10f XeXe 126-158 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10f XeXe 126-158 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141804","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t55","first_author":{},"id":141804,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141804,"related_publication":139684,"title":"Figure 10f XeXe 126-158 GeV","uuid":"9f84d9a7-634e-4c35-8c50-66f7351e8dfe"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10f PbPb 126-158 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10f PbPb 126-158 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10f PbPb 126-158 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10f PbPb 126-158 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10f PbPb 126-158 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141805","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t56","first_author":{},"id":141805,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141805,"related_publication":139684,"title":"Figure 10f PbPb 126-158 GeV","uuid":"9fc4dea3-d1b8-4182-bd95-ea8651d334dd"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10g XeXe 158-199 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10g XeXe 158-199 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10g XeXe 158-199 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10g XeXe 158-199 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10g XeXe 158-199 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141806","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t57","first_author":{},"id":141806,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141806,"related_publication":139684,"title":"Figure 10g XeXe 158-199 GeV","uuid":"dee8ff22-e6ca-401a-be6c-9ebd3d217cb4"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10g PbPb 158-199 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10g PbPb 158-199 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10g PbPb 158-199 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10g PbPb 158-199 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10g PbPb 158-199 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141807","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t58","first_author":{},"id":141807,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141807,"related_publication":139684,"title":"Figure 10g PbPb 158-199 GeV","uuid":"dba0a545-9a2b-4295-aabd-7be4c00fd259"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10h XeXe 158-199 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10h XeXe 158-199 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10h XeXe 158-199 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10h XeXe 158-199 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10h XeXe 158-199 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141808","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t59","first_author":{},"id":141808,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141808,"related_publication":139684,"title":"Figure 10h XeXe 158-199 GeV","uuid":"4495dfd0-f12a-4819-a445-666927d65718"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10h PbPb 158-199 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10h PbPb 158-199 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10h PbPb 158-199 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10h PbPb 158-199 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10h PbPb 158-199 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141809","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t60","first_author":{},"id":141809,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141809,"related_publication":139684,"title":"Figure 10h PbPb 158-199 GeV","uuid":"e6d9ee49-0c81-4ced-b0f0-3e69154d7cdd"},{"abstract":"Per-pair normalized xJ distribution in Xe+Xe collisions for selected Pb+Pb centrality and pT1 bin. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10i XeXe 158-199 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10i XeXe 158-199 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10i XeXe 158-199 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10i XeXe 158-199 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10i XeXe 158-199 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141810","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0}],"reactions":["Xe Xe --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t61","first_author":{},"id":141810,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Xe Xe --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5440.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141810,"related_publication":139684,"title":"Figure 10i XeXe 158-199 GeV","uuid":"c9e2838c-a8c7-4aff-bf49-c02b374085e6"},{"abstract":"","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2630510/Figure 10i PbPb 158-199 GeV/csv","json":"https://www.hepdata.net/download/table/ins2630510/Figure 10i PbPb 158-199 GeV/json","root":"https://www.hepdata.net/download/table/ins2630510/Figure 10i PbPb 158-199 GeV/root","yaml":"https://www.hepdata.net/download/table/ins2630510/Figure 10i PbPb 158-199 GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2630510/Figure 10i PbPb 158-199 GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"141811","creation_date":"2023-02-08","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"reactions":["Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.139684.v1/t62","first_author":{},"id":141811,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"name":"reactions","synonyms":"","value":"Pb Pb --> DIJET"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2023-07-17T09:42:08","parent_child_join":{"name":"child_datatable","parent":"139684"},"recid":141811,"related_publication":139684,"title":"Figure 10i PbPb 158-199 GeV","uuid":"dae07504-d8c1-4649-ac5b-7c1a0887a2db"}],"data_keywords":{"cmenergies":[{"gte":5440.0,"lte":5440.0},{"gte":5020.0,"lte":5020.0}],"reactions":["Xe Xe --> DIJET","XE XE --> DIJET","PB PB --> JETS X","Pb Pb --> DIJET"]},"date":"08 Feb 2023","doc_type":"publication","doi":"10.1103/PhysRevC.108.024906","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"hepdata_doi":"10.17182/hepdata.139684","id":139684,"inspire_id":"2630510","journal_info":"Phys.Rev.C 108 (2023) 024906","keywords":[{"schema":"INSPIRE","value":"parton: scattering"},{"schema":"INSPIRE","value":"dijet: momentum"},{"schema":"INSPIRE","value":"dijet: suppression"},{"schema":"INSPIRE","value":"parton: energy loss"},{"schema":"INSPIRE","value":"energy: density"},{"schema":"INSPIRE","value":"TeV"},{"schema":"INSPIRE","value":"GeV"},{"schema":"INSPIRE","value":"correlation"},{"schema":"INSPIRE","value":"fluctuation"},{"schema":"INSPIRE","value":"peripheral"},{"schema":"INSPIRE","value":"path length"},{"schema":"INSPIRE","value":"interpretation of experiments: CERN LHC Coll"},{"schema":"INSPIRE","value":"anti-kT algorithm"},{"schema":"INSPIRE","value":"interpretation of experiments: ATLAS"}],"last_updated":"2023-07-17T09:42:16","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-03-27T00:00:00","recid":139684,"subject_area":["nucl-ex","hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},{"affiliation":"Oklahoma U.","full_name":"Abbott, B."},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, K."},{"affiliation":"Brookhaven","full_name":"Abidi, S.H."},{"affiliation":"Rabat U.","full_name":"Aboulhorma, A."},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, H."},{"affiliation":"Technion","full_name":"Abreu, H."},{"affiliation":"New York U.","full_name":"Abulaiti, Y."},{"affiliation":"Chile U., Catolica","full_name":"Abusleme Hoffman, A.C."},{"affiliation":"ICTP, Trieste","full_name":"Acharya, B.S."}],"title":"Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\\sqrt{s_{NN}}$ = 5.44 TeV","total_tables":62,"type":["article"],"uuid":"6df15126-6d21-47f2-9be1-9924d32b87c6","version":1,"year":"2023"},{"abstract":"A search for flavor-changing neutral-current couplings between a top quark, an up or charm quark and a $Z$ boson is presented, using proton-proton collision data at $\\sqrt{s} = 13$ TeV collected by the ATLAS detector at the Large Hadron Collider. The analyzed dataset corresponds to an integrated luminosity of 139 fb$^{-1}$. The search targets both single-top-quark events produced as $gq\\rightarrow tZ$ (with $q = u, c$) and top-quark-pair events, with one top quark decaying through the $t \\rightarrow Zq$ channel. The analysis considers events with three leptons (electrons or muons), a $b$-tagged jet, possible additional jets, and missing transverse momentum. The data are found to be consistent with the background-only hypothesis and 95% confidence-level limits on the $t \\rightarrow Zq$ branching ratios are set, assuming only tensor operators of the Standard Model effective field theory framework contribute to the $tZq$ vertices. These are $6.2 \\times 10^{-5}$ ($13\\times 10^{-5}$) for $t\\rightarrow Zu$ ($t\\rightarrow Zc$) for a left-handed $tZq$ coupling, and $6.6 \\times 10^{-5}$ ($12\\times 10^{-5}$) in the case of a right-handed coupling. These results are interpreted as 95% CL upper limits on the strength of corresponding couplings, yielding limits for $|C_{uW}^{(13)*}|$ and $|C_{uB}^{(13)*}|$ ($|C_{uW}^{(31)}|$ and $|C_{uB}^{(31)}|$) of 0.15 (0.16), and limits for $|C_{uW}^{(23)*}|$ and $|C_{uB}^{(23)*}|$ ($|C_{uW}^{(32)}|$ and $|C_{uB}^{(32)}|$) of 0.22 (0.21), assuming a new-physics energy scale $\\Lambda_\\text{NP}$ of 1 TeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2627201/1/csv","json":"https://www.hepdata.net/download/submission/ins2627201/1/json","root":"https://www.hepdata.net/download/submission/ins2627201/1/root","yaml":"https://www.hepdata.net/download/submission/ins2627201/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2627201/1/yoda"}},"analyses":[{"analysis":"https://www.hepdata.net/record/resource/3482086?landing_page=true","filename":"workspace_tZu_LH.json","type":"HistFactory"},{"analysis":"https://www.hepdata.net/record/resource/3482087?landing_page=true","filename":"workspace_tZu_RH.json","type":"HistFactory"},{"analysis":"https://www.hepdata.net/record/resource/3482088?landing_page=true","filename":"workspace_tZc_LH.json","type":"HistFactory"},{"analysis":"https://www.hepdata.net/record/resource/3482089?landing_page=true","filename":"workspace_tZc_RH.json","type":"HistFactory"}],"arxiv_id":"arXiv:2301.11605","authors":["Aad, G.","Abbott, B.","Abbott, D.C.","Abed Abud, A.","Abeling, K.","Abhayasinghe, D.K.","Abidi, S.H.","Aboulhorma, A.","Abramowicz, H.","Abreu, H."],"collaborations":["ATLAS"],"control_number":"145074","creation_date":"2023-01-27","data":[{"abstract":"Summary of the signal strength $\\mu$ parameters obtained from the fits to extract LH and RH results for the FCNC tZu and tZc couplings. For the reference branching ratio, the most stringent limits are used.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Table 7/csv","json":"https://www.hepdata.net/download/table/ins2627201/Table 7/json","root":"https://www.hepdata.net/download/table/ins2627201/Table 7/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Table 7/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Table 7/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145906","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145906,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145906,"related_publication":145074,"title":"Table 7","uuid":"65e1f00a-7a13-4f3c-a3ff-6293b5107984"},{"abstract":"Observed and expected 95% CL limits on the FCNC $t\\rightarrow Zq$ branching ratios and the effective coupling strengths for different vertices and couplings (top eight rows). For the latter, the energy scale is assumed to be $\\Lambda_{NP}$ = 1 TeV. The bottom rows show, for the case of the FCNC $t\\rightarrow Zu$ branching ratio, the observed and expected 95% CL limits when only one of the two SRs, either SR1 or SR2, and all CRs are included in the likelihood.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Table 8/csv","json":"https://www.hepdata.net/download/table/ins2627201/Table 8/json","root":"https://www.hepdata.net/download/table/ins2627201/Table 8/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Table 8/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Table 8/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145907","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145907,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145907,"related_publication":145074,"title":"Table 8","uuid":"edd0b7d3-0c80-45ff-830a-14a38b8fa2e5"},{"abstract":"Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the SM top-quark candidate in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145908","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DM"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145908,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DM"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145908,"related_publication":145074,"title":"Figure 02a","uuid":"79a808ba-6d17-4bf5-bf2d-5d8db6457418"},{"abstract":"Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the FCNC top-quark candidate in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145909","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DM"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145909,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DM"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145909,"related_publication":145074,"title":"Figure 02b","uuid":"7106f9ca-6799-4511-854e-61672aad6367"},{"abstract":"Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the SM top-quark candidate in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 02c/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 02c/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 02c/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 02c/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 02c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145910","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DM"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145910,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DM"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145910,"related_publication":145074,"title":"Figure 02c","uuid":"d70416fc-71e8-4276-a71a-88e5ad103fa9"},{"abstract":"Comparison between data and background prediction before the fit (Pre-Fit) for the transverse momentum of the Z boson candidate in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145911","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DPT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145911,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DPT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145911,"related_publication":145074,"title":"Figure 02d","uuid":"f8f1e742-4253-4495-b8ea-112df51ad4a7"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{1}$ discriminant in the mass sideband CR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 03a/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 03a/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 03a/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 03a/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 03a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145912","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145912,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145912,"related_publication":145074,"title":"Figure 03a","uuid":"cc9838e6-cce6-49b6-a34b-b52819ff471a"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{2}^{u}$ discriminant in the mass sideband CR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 03b/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 03b/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 03b/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 03b/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 03b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145913","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145913,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145913,"related_publication":145074,"title":"Figure 03b","uuid":"389236ce-f22e-40f8-b0cf-684b64c4a92d"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{1}$ discriminant in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 03c/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 03c/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 03c/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 03c/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 03c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145914","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145914,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145914,"related_publication":145074,"title":"Figure 03c","uuid":"37a39a0f-4784-471f-a600-4c893678aac2"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{2}^{u}$ discriminant in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 03d/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 03d/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 03d/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 03d/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 03d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145915","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145915,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145915,"related_publication":145074,"title":"Figure 03d","uuid":"dfb5939e-762f-45e2-ba9a-c1f55349f61d"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{1}$ discriminant in the mass sideband CR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 04a/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 04a/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 04a/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 04a/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 04a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145916","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145916,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145916,"related_publication":145074,"title":"Figure 04a","uuid":"349efe29-0520-4cdb-b0e5-dc296a0b3a82"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{2}^{c}$ discriminant in the mass sideband CR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 04b/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 04b/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 04b/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 04b/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 04b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145917","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145917,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145917,"related_publication":145074,"title":"Figure 04b","uuid":"831c31cb-d03c-4a4e-ac3b-80353b36a365"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{1}$ discriminant in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 04c/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 04c/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 04c/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 04c/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 04c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145918","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145918,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145918,"related_publication":145074,"title":"Figure 04c","uuid":"8941822a-4af0-4c34-ab49-3e086be42e6d"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZc LH coupling extraction. The distribution is for the $D_{2}^{c}$ discriminant in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZc LH signals are also separately shown, normalized to 50 times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 04d/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 04d/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 04d/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 04d/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 04d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145919","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145919,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145919,"related_publication":145074,"title":"Figure 04d","uuid":"5d8f3fd1-dd0f-4649-85a8-dd6a638ba1d9"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the leading lepton $p_{T}$ in the $t\\bar{t}$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The last bin includes the overflow. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01a/csv","json":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01a/json","root":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01a/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01a/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145920","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DPT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145920,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DPT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145920,"related_publication":145074,"title":"Auxiliary Figure 01a","uuid":"489b6703-87cb-4228-a219-a2ea7ba64693"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the third lepton $p_{T}$ in the $t\\bar{t}$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The last bin includes the overflow. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01b/csv","json":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01b/json","root":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01b/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01b/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145921","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DPT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145921,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DPT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145921,"related_publication":145074,"title":"Auxiliary Figure 01b","uuid":"7b66e006-f825-42d9-9902-cf2080f3179c"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the leading lepton $p_{T}$ in the $t\\bar{t}Z$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The last bin includes the overflow. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01c/csv","json":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01c/json","root":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01c/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01c/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01c/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145922","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DPT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145922,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DPT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145922,"related_publication":145074,"title":"Auxiliary Figure 01c","uuid":"7f8d4652-9eca-494e-bcb8-82451a8c2590"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{1}$ discriminant in the $t\\bar{t}Z$ CR. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also shown separately, normalized to $10^{3}$ times the best fit of the signal yield. The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01d/csv","json":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01d/json","root":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01d/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01d/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Auxiliary Figure 01d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145923","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145923,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DBDT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145923,"related_publication":145074,"title":"Auxiliary Figure 01d","uuid":"eed1a7ff-60e0-4016-a528-a72a7e75c5de"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DBDT","DN/DM","DN/DPT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"publication","doi":"10.1103/PhysRevD.108.032019","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"hepdata_doi":"10.17182/hepdata.145074","id":145074,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"top: pair production"},{"schema":"INSPIRE","value":"top: single production"},{"schema":"INSPIRE","value":"Z0: associated production"},{"schema":"INSPIRE","value":"neutral current: coupling"},{"schema":"INSPIRE","value":"neutral current: flavor changing"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"operator: tensor"},{"schema":"INSPIRE","value":"transverse momentum: missing-energy"},{"schema":"INSPIRE","value":"coupling: right-handed"},{"schema":"INSPIRE","value":"scale: new physics"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"muon"},{"schema":"INSPIRE","value":"top: branching ratio: upper limit"},{"schema":"INSPIRE","value":"electron"},{"schema":"INSPIRE","value":"final state: ((n)jet 3lepton)"},{"schema":"INSPIRE","value":"charm"},{"schema":"INSPIRE","value":"left-handed"},{"schema":"INSPIRE","value":"effective field theory"},{"schema":"INSPIRE","value":"coupling constant: upper limit"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2023-12-15T10:09:17","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-15T00:00:00","recid":145074,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},{"affiliation":"Oklahoma U.","full_name":"Abbott, B."},{"affiliation":"Massachusetts U., Amherst","full_name":"Abbott, D.C."},{"affiliation":"CERN","full_name":"Abed Abud, A."},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, K."},{"affiliation":"Royal Holloway, U. of London","full_name":"Abhayasinghe, D.K."},{"affiliation":"Brookhaven","full_name":"Abidi, S.H."},{"affiliation":"Rabat U.","full_name":"Aboulhorma, A."},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, H."},{"affiliation":"Technion","full_name":"Abreu, H."}],"title":"Search for flavor-changing neutral-current couplings between the top quark and the $Z$ boson with LHC Run 2 proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","total_tables":18,"type":["article"],"uuid":"6595f18d-3ea8-45de-900c-e02b81d6be71","version":1,"year":"2023"},{"abstract":"Several extensions of the Standard Model predict the production of dark matter particles at the LHC. A search for dark matter particles produced in association with a dark Higgs boson decaying into $W^{+}W^{-}$ in the $\\ell^\\pm\\nu q \\bar q'$ final states with $\\ell=e,\\mu$ is presented. This analysis uses 139 fb$^{-1}$ of $pp$ collisions recorded by the ATLAS detector at a centre-of-mass energy of 13 TeV. The $W^\\pm \\to q\\bar q'$ decays are reconstructed from pairs of calorimeter-measured jets or from track-assisted reclustered jets, a technique aimed at resolving the dense topology from a pair of boosted quarks using jets in the calorimeter and tracking information. The observed data are found to agree with Standard Model predictions. Scenarios with dark Higgs boson masses ranging between 140 and 390 GeV are excluded.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2181868/1/csv","json":"https://www.hepdata.net/download/submission/ins2181868/1/json","root":"https://www.hepdata.net/download/submission/ins2181868/1/root","yaml":"https://www.hepdata.net/download/submission/ins2181868/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2181868/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2211.07175","authors":["Aad, G.","Abbott, B.","Abbott, D.C.","Abeling, K.","Abidi, S.H.","Aboulhorma, A.","Abramowicz, H.","Abreu, H.","Abulaiti, Y.","Abusleme Hoffman, A.C."],"collaborations":["ATLAS"],"control_number":"132484","creation_date":"2022-11-14","data":[{"abstract":"Probability of finding at least one TAR jet, where the pT-leading TAR jet passes the mWcand and D2β=1 requirements, as a function of ms. The probability is determined in a sample of signal events with mZ'=500 GeV, with the preselections applied.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=500 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=500 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=500 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=500 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=500 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144481","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144481,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144481,"related_publication":132484,"title":"Merged W Candidate Reco Efficiency (mZp=500 GeV)","uuid":"72a07897-4eff-437e-b02f-1078becccebb"},{"abstract":"Probability of finding at least one TAR jet, where the pT-leading TAR jet passes the mWcand and D2β=1 requirements, as a function of ms. The probability is determined in a sample of signal events with mZ'=1000 GeV, with the preselections applied.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1000 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1000 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1000 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1000 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1000 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144482","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144482,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144482,"related_publication":132484,"title":"Merged W Candidate Reco Efficiency (mZp=1000 GeV)","uuid":"5a452570-1d6b-471e-bd46-37712bcdecc7"},{"abstract":"Probability of finding at least one TAR jet, where the pT-leading TAR jet passes the mWcand and D2β=1 requirements, as a function of ms. The probability is determined in a sample of signal events with mZ'=1700 GeV, with the preselections applied.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1700 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1700 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1700 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1700 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=1700 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144483","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144483,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144483,"related_publication":132484,"title":"Merged W Candidate Reco Efficiency (mZp=1700 GeV)","uuid":"f19eabd3-722b-4396-a192-ed8fba140c74"},{"abstract":"Probability of finding at least one TAR jet, where the pT-leading TAR jet passes the mWcand and D2β=1 requirements, as a function of ms. The probability is determined in a sample of signal events with mZ'=2100 GeV, with the preselections applied.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=2100 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=2100 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=2100 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=2100 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Merged W Candidate Reco Efficiency (mZp=2100 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144484","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144484,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144484,"related_publication":132484,"title":"Merged W Candidate Reco Efficiency (mZp=2100 GeV)","uuid":"39049fec-52e4-48d0-a745-950d9b3efd27"},{"abstract":"Probability of finding a Whad candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of ms. The probability is determined in a sample of signal events with mZ'=500 GeV, with the preselections applied that do not pass the requirements of the merged category.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=500 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=500 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=500 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=500 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=500 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144485","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144485,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144485,"related_publication":132484,"title":"Resolved W Candidate Reco Efficiency (mZp=500 GeV)","uuid":"168eaea1-bc94-48f0-9ea3-ad55c92e7c37"},{"abstract":"Probability of finding a Whad candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of ms. The probability is determined in a sample of signal events with mZ'=1000 GeV, with the preselections applied that do not pass the requirements of the merged category.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1000 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1000 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1000 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1000 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1000 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144486","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144486,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144486,"related_publication":132484,"title":"Resolved W Candidate Reco Efficiency (mZp=1000 GeV)","uuid":"25b0318e-46f9-40b8-9109-291b4e7b6d78"},{"abstract":"Probability of finding a Whad candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of ms. The probability is determined in a sample of signal events with mZ'=1700 GeV, with the preselections applied that do not pass the requirements of the merged category.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1700 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1700 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1700 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1700 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=1700 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144487","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144487,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144487,"related_publication":132484,"title":"Resolved W Candidate Reco Efficiency (mZp=1700 GeV)","uuid":"6e561f68-78cb-490c-b540-b234f28e4c83"},{"abstract":"Probability of finding a Whad candidate reconstructed as a pair of R=0.4 PFlow jets, as a function of ms. The probability is determined in a sample of signal events with mZ'=2100 GeV, with the preselections applied that do not pass the requirements of the merged category.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=2100 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=2100 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=2100 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=2100 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Resolved W Candidate Reco Efficiency (mZp=2100 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144488","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144488,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144488,"related_publication":132484,"title":"Resolved W Candidate Reco Efficiency (mZp=2100 GeV)","uuid":"6064f897-7a2a-428a-bff5-9ac6adf3e1a3"},{"abstract":"Observed exclusion contour at 95% C.L. for the dark Higgs model in the (mZ', ms) plane for gq=0.25, gχ=1, mχ=200 GeV, and sinθ=0.01.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Observed)/csv","json":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Observed)/json","root":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Observed)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Observed)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Observed)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144489","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144489,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144489,"related_publication":132484,"title":"CLs exclusion contour (Observed)","uuid":"9ad7feaf-1e2b-4cdf-a37e-72fb9bc552f4"},{"abstract":"Expected exclusion contour at 95% C.L. for the dark Higgs model in the (mZ', ms) plane for gq=0.25, gχ=1, mχ=200 GeV, and sinθ=0.01.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected)/csv","json":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected)/json","root":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144490","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144490,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144490,"related_publication":132484,"title":"CLs exclusion contour (Expected)","uuid":"a70e8876-5322-4bfb-a844-f05d5a75eaaf"},{"abstract":"Expected+1σ exclusion contour at 95% C.L. for the dark Higgs model in the (mZ', ms) plane for gq=0.25, gχ=1, mχ=200 GeV, and sinθ=0.01.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 1 sigma)/csv","json":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 1 sigma)/json","root":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 1 sigma)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 1 sigma)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 1 sigma)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144491","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144491,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144491,"related_publication":132484,"title":"CLs exclusion contour (Expected + 1 sigma)","uuid":"44ade307-63ae-4f8a-809b-c465e37ddfce"},{"abstract":"Expected-1σ exclusion contour at 95% C.L. for the dark Higgs model in the (mZ', ms) plane for gq=0.25, gχ=1, mχ=200 GeV, and sinθ=0.01.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 1 sigma)/csv","json":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 1 sigma)/json","root":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 1 sigma)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 1 sigma)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 1 sigma)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144492","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144492,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144492,"related_publication":132484,"title":"CLs exclusion contour (Expected - 1 sigma)","uuid":"f9555872-b13f-4f19-8281-59a8cc4174f2"},{"abstract":"Expected+2σ exclusion contour at 95% C.L. for the dark Higgs model in the (mZ', ms) plane for gq=0.25, gχ=1, mχ=200 GeV, and sinθ=0.01.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 2 sigma)/csv","json":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 2 sigma)/json","root":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 2 sigma)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 2 sigma)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected + 2 sigma)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144493","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144493,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144493,"related_publication":132484,"title":"CLs exclusion contour (Expected + 2 sigma)","uuid":"3d81aa6a-b8ef-4eab-9182-d2d0439f3fcb"},{"abstract":"Expected-2σ exclusion contour at 95% C.L. for the dark Higgs model in the (mZ', ms) plane for gq=0.25, gχ=1, mχ=200 GeV, and sinθ=0.01.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 2 sigma)/csv","json":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 2 sigma)/json","root":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 2 sigma)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 2 sigma)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/CLs exclusion contour (Expected - 2 sigma)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144494","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144494,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144494,"related_publication":132484,"title":"CLs exclusion contour (Expected - 2 sigma)","uuid":"46c206d6-f997-41f8-8846-de15c7ade756"},{"abstract":"Observed upper limits at 95% C.L. on σ(pp → s χχ) × B(s → W± W∓) for mZ'=0.5 TeV as a function of ms. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the σ(pp → s χχ) × B(s → W± W∓) process for mZ'=0.5 TeV, shown in dashed blue.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=500 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=500 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=500 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=500 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=500 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144495","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144495,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144495,"related_publication":132484,"title":"Upper limits on mu (mZp=500 GeV)","uuid":"f428f266-a18f-47da-a2fb-3f0599069b2f"},{"abstract":"Observed upper limits at 95% C.L. on σ(pp → s χχ) × B(s → W± W∓) for mZ'=1 TeV as a function of ms. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the σ(pp → s χχ) × B(s → W± W∓) process for mZ'=1 TeV, shown in dashed blue.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1000 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1000 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1000 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1000 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1000 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144496","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144496,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144496,"related_publication":132484,"title":"Upper limits on mu (mZp=1000 GeV)","uuid":"54346f17-c614-4218-89fb-e4caee1e041b"},{"abstract":"Observed upper limits at 95% C.L. on σ(pp → s χχ) × B(s → W± W∓) for mZ'=1.7 TeV as a function of ms. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the σ(pp → s χχ) × B(s → W± W∓) process for mZ'=1.7 TeV, shown in dashed blue.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1700 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1700 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1700 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1700 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=1700 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144497","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144497,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144497,"related_publication":132484,"title":"Upper limits on mu (mZp=1700 GeV)","uuid":"ca23b407-188d-4cf1-ac0f-c764e93701a2"},{"abstract":"Observed upper limits at 95% C.L. on σ(pp → s χχ) × B(s → W± W∓) for mZ'=2.1 TeV as a function of ms. The expected limits, varied up and down by one and two standard deviations, are shown as green and yellow bands, respectively. The observed and expected limits are compared to the theoretical LO cross section for the σ(pp → s χχ) × B(s → W± W∓) process for mZ'=2.1 TeV, shown in dashed blue.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=2100 GeV)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=2100 GeV)/json","root":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=2100 GeV)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=2100 GeV)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Upper limits on mu (mZp=2100 GeV)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144498","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144498,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144498,"related_publication":132484,"title":"Upper limits on mu (mZp=2100 GeV)","uuid":"c4057179-fcf2-4af9-b834-729042e6f822"},{"abstract":"Data overlaid on SM background yields stacked in each SR and CR category after the fit to data ('Post-fit'). The yields in the SR are broken down into their contributions to the individual bins. The maximum-likelihood estimators are set to the conditional values of the CR-only fit, and propagated to SR and CRs.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Data and MC in all regions (CR-only fit)/csv","json":"https://www.hepdata.net/download/table/ins2181868/Data and MC in all regions (CR-only fit)/json","root":"https://www.hepdata.net/download/table/ins2181868/Data and MC in all regions (CR-only fit)/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Data and MC in all regions (CR-only fit)/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Data and MC in all regions (CR-only fit)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144499","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t19","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144499,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144499,"related_publication":132484,"title":"Data and MC in all regions (CR-only fit)","uuid":"6168e251-c2e8-440e-bdbe-852c5c565e8d"},{"abstract":"Dominant sources of uncertainty for three dark Higgs scenarios after the fit to data. The uncertainties are quantified in terms of their contribution to the fitted signal uncertainty that is expressed relative to the theory prediction. Three representative dark Higgs signal scenarios with gq=0.25, gχ=1.0, sinθ=0.01 and mχ=200 GeV are considered, which are indicated using the (mZ', ms) format in units of GeV in the table columns.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Sources of uncertainty/csv","json":"https://www.hepdata.net/download/table/ins2181868/Sources of uncertainty/json","root":"https://www.hepdata.net/download/table/ins2181868/Sources of uncertainty/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Sources of uncertainty/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Sources of uncertainty/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144500","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t20","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144500,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144500,"related_publication":132484,"title":"Sources of uncertainty","uuid":"239d186d-6711-4dfa-a887-811bb9c0898d"},{"abstract":"Cumulative efficiencies in the merged category for three representative dark Higgs signal scenarios with gq=0.25, gχ=1.0, sinθ=0.01, mZ' = 1 TeV, and mχ=200 GeV considering s→W(ℓν)W(qq) decays only.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Merged SR cutflow efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2181868/Merged SR cutflow efficiencies/json","root":"https://www.hepdata.net/download/table/ins2181868/Merged SR cutflow efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Merged SR cutflow efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Merged SR cutflow efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144501","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t21","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144501,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144501,"related_publication":132484,"title":"Merged SR cutflow efficiencies","uuid":"bc9b4927-d36b-4a6f-8b63-eb5cd86ce247"},{"abstract":"Cumulative efficiencies in the resolved category for three representative dark Higgs signal scenarios with gq=0.25, gχ=1.0, sinθ=0.01, mZ' = 1 TeV, and mχ=200 GeV considering s→W(ℓν)W(qq) decays only.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Resolved SR cutflow efficiencies/csv","json":"https://www.hepdata.net/download/table/ins2181868/Resolved SR cutflow efficiencies/json","root":"https://www.hepdata.net/download/table/ins2181868/Resolved SR cutflow efficiencies/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Resolved SR cutflow efficiencies/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Resolved SR cutflow efficiencies/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144502","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t22","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144502,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144502,"related_publication":132484,"title":"Resolved SR cutflow efficiencies","uuid":"5447a7a3-cff7-4ba1-80f0-382857667cfb"},{"abstract":"Theoretical cross section for σ(pp → sχχ) × B(s → W±W∓) for each of the dark Higgs signal points at mZ\u2032 ={300, 350, 400, 500, 750} GeV, with gq = 0.25, gχ = 1.0, sinθ = 0.01, mZ\u2032 = 1 TeV , and mχ = 200 GeV. Also shown are experimentally excluded cross sections of σ(pp → sχχ) × B(s → W±W∓) (Obs.) together with the expectations (Exp.) varied up and down by one standard deviation (±1σ).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={300, 350, 400, 500, 750} GeV/csv","json":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={300, 350, 400, 500, 750} GeV/json","root":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={300, 350, 400, 500, 750} GeV/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={300, 350, 400, 500, 750} GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={300, 350, 400, 500, 750} GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144503","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t23","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144503,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144503,"related_publication":132484,"title":"Excluded cross sections at mZp={300, 350, 400, 500, 750} GeV","uuid":"837075f1-c053-48d5-a04d-13695a1120ca"},{"abstract":"Theoretical cross section for σ(pp → sχχ) × B(s → W±W∓) for each of the dark Higgs signal points at mZ\u2032 ={1000, 1700} GeV, with gq = 0.25, gχ = 1.0, sinθ = 0.01, mZ\u2032 = 1 TeV , and mχ = 200 GeV. Also shown are experimentally excluded cross sections of σ(pp → sχχ) × B(s → W±W∓) (Obs.) together with the expectations (Exp.) varied up and down by one standard deviation (±1σ).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={1000, 1700} GeV/csv","json":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={1000, 1700} GeV/json","root":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={1000, 1700} GeV/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={1000, 1700} GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={1000, 1700} GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144504","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t24","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144504,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144504,"related_publication":132484,"title":"Excluded cross sections at mZp={1000, 1700} GeV","uuid":"3b72451c-9694-4496-a38c-79f93b7c062a"},{"abstract":"Theoretical cross section for σ(pp → sχχ) × B(s → W±W∓) for each of the dark Higgs signal points at mZ\u2032 ={2100, 2500, 2900, 3300} GeV, with gq = 0.25, gχ = 1.0, sinθ = 0.01, mZ\u2032 = 1 TeV , and mχ = 200 GeV. Also shown are experimentally excluded cross sections of σ(pp → sχχ) × B(s → W±W∓) (Obs.) together with the expectations (Exp.) varied up and down by one standard deviation (±1σ).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={2100, 2500, 2900, 3300} GeV/csv","json":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={2100, 2500, 2900, 3300} GeV/json","root":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={2100, 2500, 2900, 3300} GeV/root","yaml":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={2100, 2500, 2900, 3300} GeV/yaml","yoda":"https://www.hepdata.net/download/table/ins2181868/Excluded cross sections at mZp={2100, 2500, 2900, 3300} GeV/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"144505","creation_date":"2022-11-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.132484.v1/t25","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":144505,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"name":"reactions","synonyms":"","value":"P P --> W W X"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"phrases","synonyms":"","value":"Dark Higgs"},{"name":"phrases","synonyms":"","value":"Simplified Model"},{"name":"phrases","synonyms":"","value":"Spin-1 Mediator"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2023-09-27T00:15:47","parent_child_join":{"name":"child_datatable","parent":"132484"},"recid":144505,"related_publication":132484,"title":"Excluded cross sections at mZp={2100, 2500, 2900, 3300} GeV","uuid":"9ce9ae4c-c977-47db-aa07-b22a6338d74f"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Dark Matter","Proton-Proton Scattering","Spin-1 Mediator","Simplified Model","Dark Higgs"],"reactions":["P P --> W W X"]},"date":"14 Nov 2022","doc_type":"publication","doi":"10.1007/JHEP07(2023)116","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"hepdata_doi":"10.17182/hepdata.132484","id":132484,"inspire_id":"2181868","journal_info":"JHEP 07 (2023) 116","keywords":[{"source":"author","value":"Dark Matter"},{"source":"author","value":"Hadron-Hadron Scattering"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"dark matter: associated production"},{"schema":"INSPIRE","value":"Higgs particle: associated production"},{"schema":"INSPIRE","value":"Higgs particle: decay modes"},{"schema":"INSPIRE","value":"W: pair production"},{"schema":"INSPIRE","value":"Higgs particle: mass: lower limit"},{"schema":"INSPIRE","value":"hidden sector"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"final state: ((n)jet lepton)"},{"schema":"INSPIRE","value":"electron"},{"schema":"INSPIRE","value":"muon"},{"schema":"INSPIRE","value":"calorimeter"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"topology"},{"schema":"INSPIRE","value":"boosted particle"},{"schema":"INSPIRE","value":"channel cross section: branching ratio: upper limit"},{"schema":"INSPIRE","value":"track data analysis: jet"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2023-09-27T00:15:51","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-11T00:00:00","recid":132484,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},{"affiliation":"U. Oklahoma, Norman","full_name":"Abbott, B."},{"affiliation":"Massachusetts U., Amherst","full_name":"Abbott, D.C."},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, K."},{"affiliation":"Brookhaven","full_name":"Abidi, S.H."},{"affiliation":"Rabat U.","full_name":"Aboulhorma, A."},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, H."},{"affiliation":"Technion","full_name":"Abreu, H."},{"affiliation":"City Coll., N.Y.","full_name":"Abulaiti, Y."},{"affiliation":"Chile U., Catolica","full_name":"Abusleme Hoffman, A.C."}],"title":"Search for dark matter produced in association with a dark Higgs boson decaying into $W^{+}W^{-}$ in the one-lepton final state at $\\sqrt{s}$=13 TeV using 139 fb$^{-1}$ of $pp$ collisions recorded with the ATLAS detector","total_tables":25,"type":["article"],"uuid":"2a2d4ff0-ed3e-4580-aafc-403bf626d5d2","version":1,"year":"2023"},{"abstract":"Inclusive and differential measurements of the top-antitop ($t\\bar{t}$) charge asymmetry $A_\\text{C}^{t\\bar{t}}$ and the leptonic asymmetry $A_\\text{C}^{\\ell\\bar{\\ell}}$ are presented in proton-proton collisions at $\\sqrt{s} = 13$ TeV recorded by the ATLAS experiment at the CERN Large Hadron Collider. The measurement uses the complete Run 2 dataset, corresponding to an integrated luminosity of 139 fb$^{-1}$, combines data in the single-lepton and dilepton channels, and employs reconstruction techniques adapted to both the resolved and boosted topologies. A Bayesian unfolding procedure is performed to correct for detector resolution and acceptance effects. The combined inclusive $t\\bar{t}$ charge asymmetry is measured to be $A_\\text{C}^{t\\bar{t}} = 0.0068 \\pm 0.0015$, which differs from zero by 4.7 standard deviations. Differential measurements are performed as a function of the invariant mass, transverse momentum and longitudinal boost of the $t\\bar{t}$ system. Both the inclusive and differential measurements are found to be compatible with the Standard Model predictions, at next-to-next-to-leading order in quantum chromodynamics perturbation theory with next-to-leading-order electroweak corrections. The measurements are interpreted in the framework of the Standard Model effective field theory, placing competitive bounds on several Wilson coefficients.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2141752/1/csv","json":"https://www.hepdata.net/download/submission/ins2141752/1/json","root":"https://www.hepdata.net/download/submission/ins2141752/1/root","yaml":"https://www.hepdata.net/download/submission/ins2141752/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2141752/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2208.12095","authors":["Aad, G.","Abbott, B.","Abbott, D.C.","Abeling, K.","Abidi, S.H.","Aboulhorma, A.","Abramowicz, H.","Abreu, H.","Abulaiti, Y.","Abusleme Hoffman, A.C."],"collaborations":["ATLAS"],"control_number":"132116","creation_date":"2022-08-25","data":[{"abstract":"- - - - - - - - Overview of HEPData Record - - - - - - - -
Results: Bounds on the Wilson coefficients: Ranking of systematic uncertainties: Inclusive:$A_C^{t\\bar{t}}$ $A_C^{t\\bar{t}}$ vs $\\beta_{z,t\\bar{t}}$: $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$: $A_C^{t\\bar{t}}$ vs $p_{T,t\\bar{t}}$: Inclusive leptonic:$A_C^{\\ell\\bar{\\ell}}$ $A_C^{\\ell\\bar{\\ell}}$ vs $\\beta_{z,\\ell\\bar{\\ell}}$ $A_C^{\\ell\\bar{\\ell}}$ vs $m_{\\ell\\bar{\\ell}}$ $A_C^{\\ell\\bar{\\ell}}$ vs $p_{T,\\ell\\bar{\\ell}}$ \nNP correlations: Covariance matrices: ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Table of contents/csv","json":"https://www.hepdata.net/download/table/ins2141752/Table of contents/json","root":"https://www.hepdata.net/download/table/ins2141752/Table of contents/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Table of contents/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Table of contents/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133083","creation_date":"2022-08-25","data_keywords":{"cmenergies":[]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t1","first_author":{},"id":133083,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133083,"related_publication":132116,"title":"Table of contents","uuid":"5971a101-ba51-4a13-ba67-bcab11fb1e6f"},{"abstract":"The unfolded inclusive charge asymmetry. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed, and the impact of the linear term of the Wilson coefficient on the $A_C^{t\\bar{t}}$ prediction is shown for two different values. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry inclusive/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry inclusive/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry inclusive/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry inclusive/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry inclusive/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133084","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t2","first_author":{},"id":133084,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133084,"related_publication":132116,"title":"Results for charge asymmetry inclusive","uuid":"8fe3ddad-b0ff-45c0-a095-56bd643bbc92"},{"abstract":"The unfolded differential charge asymmetry as a function of the invariant mass of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed, and the impact of the linear term of the Wilson coefficient on the $A_C^{t\\bar{t}}$ prediction is shown for two different values. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature. ","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs mtt/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs mtt/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs mtt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs mtt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs mtt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133085","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t3","first_author":{},"id":133085,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133085,"related_publication":132116,"title":"Results for charge asymmetry vs mtt","uuid":"d85cd81b-49c9-4227-a360-df19a4a3eb10"},{"abstract":"The unfolded differential charge asymmetry as a function of the transverse momentum of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs pttt/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs pttt/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs pttt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs pttt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs pttt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133086","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t4","first_author":{},"id":133086,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133086,"related_publication":132116,"title":"Results for charge asymmetry vs pttt","uuid":"5e3c255f-7657-4c84-a2d0-df68646c7a7a"},{"abstract":"The unfolded differential charge asymmetry as a function of the longitudinal boost of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs betatt/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs betatt/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs betatt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs betatt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for charge asymmetry vs betatt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133087","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t5","first_author":{},"id":133087,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133087,"related_publication":132116,"title":"Results for charge asymmetry vs betatt","uuid":"99fd32a7-5118-483e-b31c-59a813e348dc"},{"abstract":"The unfolded inclusive leptonic asymmetry. The unfolded $A_C^{\\ell\\bar{\\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\\Delta |\\eta_{\\ell\\bar{\\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry inclusive/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry inclusive/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry inclusive/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry inclusive/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry inclusive/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133088","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t6","first_author":{},"id":133088,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133088,"related_publication":132116,"title":"Results for leptonic charge asymmetry inclusive","uuid":"445b4420-5492-4c0d-a57e-0c73ba22dcad"},{"abstract":"The unfolded differential leptonic asymmetry as a function of the invariant mass of the di-lepton pair. The unfolded $A_C^{\\ell\\bar{\\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\\Delta |\\eta_{\\ell\\bar{\\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs mll/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs mll/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs mll/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs mll/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs mll/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133089","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t7","first_author":{},"id":133089,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133089,"related_publication":132116,"title":"Results for leptonic charge asymmetry vs mll","uuid":"a9e91c8d-9fd5-4c68-83f8-ed238e0bcd22"},{"abstract":"The unfolded differential leptonic asymmetry as a function of the transverse momentum of the di-lepton pair. The unfolded $A_C^{\\ell\\bar{\\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\\Delta |\\eta_{\\ell\\bar{\\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs ptll/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs ptll/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs ptll/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs ptll/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs ptll/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133090","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t8","first_author":{},"id":133090,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133090,"related_publication":132116,"title":"Results for leptonic charge asymmetry vs ptll","uuid":"a19c391e-30c6-4176-99df-08514af0206a"},{"abstract":"The unfolded differential leptonic asymmetry as a function of the longitudinal boost of the di-lepton pair. The unfolded $A_C^{\\ell\\bar{\\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\\Delta |\\eta_{\\ell\\bar{\\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs betall/csv","json":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs betall/json","root":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs betall/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs betall/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Results for leptonic charge asymmetry vs betall/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133091","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t9","first_author":{},"id":133091,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133091,"related_publication":132116,"title":"Results for leptonic charge asymmetry vs betall","uuid":"96a140fc-b3aa-4f0c-ba2b-6dd8f91c3b26"},{"abstract":"Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\\bar{t}}$ inclusive measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry inclusive/csv","json":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry inclusive/json","root":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry inclusive/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry inclusive/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry inclusive/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133092","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t10","first_author":{},"id":133092,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133092,"related_publication":132116,"title":"Bounds on Wilson coefficients charge asymmetry inclusive","uuid":"0f41491f-d879-499b-9db1-830c43fafb70"},{"abstract":"Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry vs mtt/csv","json":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry vs mtt/json","root":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry vs mtt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry vs mtt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Bounds on Wilson coefficients charge asymmetry vs mtt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133093","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t11","first_author":{},"id":133093,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"CLS"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133093,"related_publication":132116,"title":"Bounds on Wilson coefficients charge asymmetry vs mtt","uuid":"6d5ae7f6-f682-473f-b857-3a00ee8c06aa"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry inclusive/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry inclusive/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry inclusive/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry inclusive/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry inclusive/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133094","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t12","first_author":{},"id":133094,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133094,"related_publication":132116,"title":"NP ranking charge asymmetry inclusive","uuid":"cd51f139-44a8-4da6-b1b1-e32ecf0e3d8c"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $\\beta_{z,t\\bar{t}}$ measurement for $\\beta_{z,t\\bar{t}}$ $\\in$ [0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 0/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 0/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 0/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 0/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 0/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133095","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t13","first_author":{},"id":133095,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133095,"related_publication":132116,"title":"NP ranking charge asymmetry vs betatt bin 0","uuid":"01112ae4-c724-447e-b325-37bf2fcaff88"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $\\beta_{z,t\\bar{t}}$ measurement for $\\beta_{z,t\\bar{t}}$ $\\in$ [0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 1/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 1/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 1/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133096","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t14","first_author":{},"id":133096,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133096,"related_publication":132116,"title":"NP ranking charge asymmetry vs betatt bin 1","uuid":"ca3cc4c7-5ded-4041-90cf-ef2264a19a34"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $\\beta_{z,t\\bar{t}}$ measurement for $\\beta_{z,t\\bar{t}}$ $\\in$ [0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 2/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 2/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 2/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133097","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t15","first_author":{},"id":133097,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133097,"related_publication":132116,"title":"NP ranking charge asymmetry vs betatt bin 2","uuid":"68a0e5ef-9a42-41d2-8095-5c71c932ddcb"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $\\beta_{z,t\\bar{t}}$ measurement for $\\beta_{z,t\\bar{t}}$ $\\in$ [0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 3/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 3/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 3/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs betatt bin 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133098","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t16","first_author":{},"id":133098,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133098,"related_publication":132116,"title":"NP ranking charge asymmetry vs betatt bin 3","uuid":"197bd560-cfcd-44e2-8636-29a85a462503"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement for $m_{t\\bar{t}}$ < 500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 0/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 0/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 0/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 0/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 0/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133099","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t17","first_author":{},"id":133099,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133099,"related_publication":132116,"title":"NP ranking charge asymmetry vs mtt bin 0","uuid":"93f20fc3-a920-4b6b-8464-7a002d1cb079"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement for $m_{t\\bar{t}}$ $\\in$ [500,750] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 1/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 1/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 1/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133100","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t18","first_author":{},"id":133100,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133100,"related_publication":132116,"title":"NP ranking charge asymmetry vs mtt bin 1","uuid":"9b94d546-77e7-4d91-9bc1-ff979a047626"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement for $m_{t\\bar{t}}$ $\\in$ [750,1000] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 2/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 2/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 2/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133101","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t19","first_author":{},"id":133101,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133101,"related_publication":132116,"title":"NP ranking charge asymmetry vs mtt bin 2","uuid":"d23f0915-9596-4a92-8de8-0a74bd9d1023"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement for $m_{t\\bar{t}}$ $\\in$ [1000,1500] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 3/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 3/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 3/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133102","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t20","first_author":{},"id":133102,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133102,"related_publication":132116,"title":"NP ranking charge asymmetry vs mtt bin 3","uuid":"00d2a45f-3cf8-424f-a17f-5147bde68713"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement for $m_{t\\bar{t}}$ > 1500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 4/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 4/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 4/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs mtt bin 4/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133103","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t21","first_author":{},"id":133103,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133103,"related_publication":132116,"title":"NP ranking charge asymmetry vs mtt bin 4","uuid":"29b7f157-88f9-4c8a-acf9-d4967027ad50"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $p_{T,t\\bar{t}}$ measurement for $p_{T,t\\bar{t}}$ < 30 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 0/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 0/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 0/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 0/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 0/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133104","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t22","first_author":{},"id":133104,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133104,"related_publication":132116,"title":"NP ranking charge asymmetry vs pttt bin 0","uuid":"5cbab815-3310-4992-822d-414230b168e6"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $p_{T,t\\bar{t}}$ measurement for $p_{T,t\\bar{t}}$ $\\in$ [30,120] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 1/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 1/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 1/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133105","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t23","first_author":{},"id":133105,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133105,"related_publication":132116,"title":"NP ranking charge asymmetry vs pttt bin 1","uuid":"0845a90e-1b5a-407a-9f18-bb591cbb8e45"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\\bar{t}}$ vs $p_{T,t\\bar{t}}$ measurement for $p_{T,t\\bar{t}}$ > 120 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 2/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 2/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 2/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking charge asymmetry vs pttt bin 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133106","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t24","first_author":{},"id":133106,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133106,"related_publication":132116,"title":"NP ranking charge asymmetry vs pttt bin 2","uuid":"3ec7fd86-05a0-4584-9607-3865b7115a32"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry inclusive/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry inclusive/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry inclusive/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry inclusive/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry inclusive/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133107","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t25","first_author":{},"id":133107,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133107,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry inclusive","uuid":"ccea9dcc-5065-40dc-b745-8f57f45a711b"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $\\beta_{z,\\ell\\bar{\\ell}}$ measurement for $\\beta_{z,\\ell\\bar{\\ell}}$ $\\in$[0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 0/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 0/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 0/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 0/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 0/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133108","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t26","first_author":{},"id":133108,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133108,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs betall bin 0","uuid":"af55d3fb-5da1-4419-81e2-94d6cb3e7cee"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $\\beta_{z,\\ell\\bar{\\ell}}$ measurement for $\\beta_{z,\\ell\\bar{\\ell}}$ $\\in$[0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 1/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 1/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 1/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133109","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t27","first_author":{},"id":133109,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133109,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs betall bin 1","uuid":"389c9d16-c646-4844-af02-fa87d6c11290"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $\\beta_{z,\\ell\\bar{\\ell}}$ measurement for $\\beta_{z,\\ell\\bar{\\ell}}$ $\\in$[0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 2/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 2/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 2/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133110","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t28","first_author":{},"id":133110,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133110,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs betall bin 2","uuid":"ca7a2031-da3f-4c9d-8215-199c7b6541e4"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $\\beta_{z,\\ell\\bar{\\ell}}$ measurement for $\\beta_{z,\\ell\\bar{\\ell}}$ $\\in$[0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 3/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 3/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 3/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs betall bin 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133111","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t29","first_author":{},"id":133111,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133111,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs betall bin 3","uuid":"4ff8f14f-770a-4df4-b093-2e4d11316352"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $m_{\\ell\\bar{\\ell}}$ measurement for $m_{\\ell\\bar{\\ell}}$ < 200 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 0/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 0/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 0/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 0/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 0/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133112","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t30","first_author":{},"id":133112,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133112,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs mll bin 0","uuid":"3d8e9bdc-c4b8-43a2-a64d-b1ee549300d5"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $m_{\\ell\\bar{\\ell}}$ measurement for $m_{\\ell\\bar{\\ell}}$ $\\in$ [200,300] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 1/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 1/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 1/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133113","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t31","first_author":{},"id":133113,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133113,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs mll bin 1","uuid":"61e1fdd1-8f4d-4c33-b2c6-1fadb9ceacb1"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $m_{\\ell\\bar{\\ell}}$ measurement for $m_{\\ell\\bar{\\ell}}$ $\\in$ [300,400] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 2/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 2/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 2/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133114","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t32","first_author":{},"id":133114,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133114,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs mll bin 2","uuid":"2fa4577f-cf22-467f-bd48-2dcc8fffedee"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $m_{\\ell\\bar{\\ell}}$ measurement for $m_{\\ell\\bar{\\ell}}$ > 400 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 3/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 3/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 3/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs mll bin 3/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133115","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t33","first_author":{},"id":133115,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133115,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs mll bin 3","uuid":"404cdf61-483a-47c9-9fab-25eddc6248ae"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $p_{T,\\ell\\bar{\\ell}}$ measurement for $p_{T,\\ell\\bar{\\ell}}$ < 20 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 0/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 0/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 0/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 0/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 0/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133116","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t34","first_author":{},"id":133116,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133116,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs ptll bin 0","uuid":"008ae15b-7a0e-4a16-9a38-0c8b6207293e"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $p_{T,\\ell\\bar{\\ell}}$ measurement for $p_{T,\\ell\\bar{\\ell}}$ $\\in$ [20, 70] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 1/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 1/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 1/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 1/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133117","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t35","first_author":{},"id":133117,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133117,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs ptll bin 1","uuid":"65ed44ee-f99a-45b3-a212-46d999d87884"},{"abstract":"Ranking of the systematic uncertainties with marginalisation for the $A_C^{\\ell\\ell}$ vs $p_{T,\\ell\\bar{\\ell}}$ measurement for $p_{T,\\ell\\bar{\\ell}}$ > 70 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 2/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 2/json","root":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 2/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP ranking leptonic charge asymmetry vs ptll bin 2/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133118","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t36","first_author":{},"id":133118,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133118,"related_publication":132116,"title":"NP ranking leptonic charge asymmetry vs ptll bin 2","uuid":"f7ef2642-22fe-4333-9c61-256d3d7981dd"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{t\\bar{t}}$ inclusive measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry inclusive/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry inclusive/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry inclusive/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry inclusive/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry inclusive/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133119","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t37","first_author":{},"id":133119,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133119,"related_publication":132116,"title":"NP correlations charge asymmetry inclusive","uuid":"64461d10-a4e4-4019-be3e-536bbe8a0e6d"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs mtt/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs mtt/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs mtt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs mtt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs mtt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133120","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t38","first_author":{},"id":133120,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133120,"related_publication":132116,"title":"NP correlations charge asymmetry vs mtt","uuid":"922a4ee5-f365-437a-acb9-5f9d237a8021"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{t\\bar{t}}$ vs $p_{T,t\\bar{t}}$ measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs pttt/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs pttt/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs pttt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs pttt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs pttt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133121","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t39","first_author":{},"id":133121,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133121,"related_publication":132116,"title":"NP correlations charge asymmetry vs pttt","uuid":"a0f80af3-0c39-4275-b6de-74729d8f237f"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{t\\bar{t}}$ vs $\\beta_{z,t\\bar{t}}$ measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs betatt/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs betatt/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs betatt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs betatt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations charge asymmetry vs betatt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133122","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t40","first_author":{},"id":133122,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133122,"related_publication":132116,"title":"NP correlations charge asymmetry vs betatt","uuid":"0dc1d83e-8e4e-4a44-9349-de6fe2f9f99d"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{\\ell\\ell}$ inclusive measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry inclusive/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry inclusive/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry inclusive/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry inclusive/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry inclusive/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133123","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t41","first_author":{},"id":133123,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133123,"related_publication":132116,"title":"NP correlations leptonic charge asymmetry inclusive","uuid":"12b0df6a-dc17-4730-8c09-3e8f60e1a033"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{\\ell\\ell}$ vs $m_{\\ell\\bar{\\ell}}$ measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs mll/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs mll/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs mll/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs mll/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs mll/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133124","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t42","first_author":{},"id":133124,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133124,"related_publication":132116,"title":"NP correlations leptonic charge asymmetry vs mll","uuid":"2ca2561e-8f86-4675-8c75-6971a8f5b524"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{\\ell\\ell}$ vs $p_{T,\\ell\\bar{\\ell}}$ measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs ptll/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs ptll/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs ptll/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs ptll/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs ptll/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133125","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t43","first_author":{},"id":133125,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133125,"related_publication":132116,"title":"NP correlations leptonic charge asymmetry vs ptll","uuid":"8962e227-f75d-4b75-9900-a3929872d8f8"},{"abstract":"Post-marginalisation correlation coefficients $\\rho_{ij}$ of nuisance parameters for the $A_C^{\\ell\\ell}$ vs $\\beta_{z,\\ell\\bar{\\ell}}$ measurement. Only $|\\rho_{ij}| > 0.05$ values are included.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs betall/csv","json":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs betall/json","root":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs betall/root","yaml":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs betall/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/NP correlations leptonic charge asymmetry vs betall/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133126","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t44","first_author":{},"id":133126,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133126,"related_publication":132116,"title":"NP correlations leptonic charge asymmetry vs betall","uuid":"b14d3920-0c21-4fcc-bc47-de4aa7eaead6"},{"abstract":"Covariance matrix for the $A_C^{t\\bar{t}}$ vs $m_{t\\bar{t}}$ measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs mtt/csv","json":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs mtt/json","root":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs mtt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs mtt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs mtt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133127","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t45","first_author":{},"id":133127,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133127,"related_publication":132116,"title":"Covariance matrix charge asymmetry vs mtt","uuid":"c4a33555-f6f6-41a5-b891-c2b0cd9d5fe4"},{"abstract":"Covariance matrix for the $A_C^{t\\bar{t}}$ vs $p_{T,t\\bar{t}}$ measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs pttt/csv","json":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs pttt/json","root":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs pttt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs pttt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs pttt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133128","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t46","first_author":{},"id":133128,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133128,"related_publication":132116,"title":"Covariance matrix charge asymmetry vs pttt","uuid":"b7c0d896-3467-4271-9eb8-421fec5ab88e"},{"abstract":"Covariance matrix for the $A_C^{t\\bar{t}}$ vs $\\beta_{z,t\\bar{t}}$ measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs betatt/csv","json":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs betatt/json","root":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs betatt/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs betatt/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix charge asymmetry vs betatt/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133129","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Charge Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t47","first_author":{},"id":133129,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Charge Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133129,"related_publication":132116,"title":"Covariance matrix charge asymmetry vs betatt","uuid":"f3ecb7b3-30df-4456-ab93-1bac0ae90a5b"},{"abstract":"Covariance matrix for the $A_C^{\\ell\\ell}$ vs $m_{\\ell\\bar{\\ell}}$ measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs mll/csv","json":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs mll/json","root":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs mll/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs mll/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs mll/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133130","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t48","first_author":{},"id":133130,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133130,"related_publication":132116,"title":"Covariance matrix leptonic charge asymmetry vs mll","uuid":"b8f82cec-b98a-4aa6-abba-12fc5b4e7be9"},{"abstract":"Covariance matrix for the $A_C^{\\ell\\ell}$ vs $p_{T,\\ell\\bar{\\ell}}$ measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs ptll/csv","json":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs ptll/json","root":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs ptll/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs ptll/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs ptll/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133131","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t49","first_author":{},"id":133131,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133131,"related_publication":132116,"title":"Covariance matrix leptonic charge asymmetry vs ptll","uuid":"a9c4d2d7-761c-41ea-920b-07b27107f22a"},{"abstract":"Covariance matrix for the $A_C^{\\ell\\ell}$ vs $\\beta_{z,\\ell\\bar{\\ell}}$ measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs betall/csv","json":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs betall/json","root":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs betall/root","yaml":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs betall/yaml","yoda":"https://www.hepdata.net/download/table/ins2141752/Covariance matrix leptonic charge asymmetry vs betall/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"133132","creation_date":"2022-08-25","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["ASYM"],"phrases":["Top","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"datatable","doi":"10.17182/hepdata.132116.v1/t50","first_author":{},"id":133132,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"name":"observables","synonyms":"","value":"ASYM"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Asymmetry Measurement"},{"name":"phrases","synonyms":"","value":"Leptonic Asymmetry"},{"name":"reactions","synonyms":"","value":"PP --> TOP TOPBAR"}],"last_updated":"2022-09-02T14:08:09","parent_child_join":{"name":"child_datatable","parent":"132116"},"recid":133132,"related_publication":132116,"title":"Covariance matrix leptonic charge asymmetry vs betall","uuid":"f9f4aa07-9b93-4a83-8e4d-7a36e86f2d8f"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS","ASYM"],"phrases":["Top","Charge Asymmetry","Leptonic Asymmetry","Asymmetry Measurement"],"reactions":["PP --> TOP TOPBAR"]},"date":"25 Aug 2022","doc_type":"publication","doi":"10.1007/JHEP08(2023)077","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"hepdata_doi":"10.17182/hepdata.132116","id":132116,"inspire_id":"2141752","journal_info":"JHEP 08 (2023) 077","keywords":[{"source":"author","value":"Hadron-Hadron Scattering"},{"source":"author","value":"Top Physics"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"top: pair production"},{"schema":"INSPIRE","value":"charge: asymmetry"},{"schema":"INSPIRE","value":"detector: resolution"},{"schema":"INSPIRE","value":"electroweak interaction: correction"},{"schema":"INSPIRE","value":"quantum chromodynamics: perturbation theory"},{"schema":"INSPIRE","value":"charge: asymmetry: measured"},{"schema":"INSPIRE","value":"perturbation theory: higher-order"},{"schema":"INSPIRE","value":"higher-order: 1"},{"schema":"INSPIRE","value":"higher-order: 2"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"final state: ((n)jet dilepton)"},{"schema":"INSPIRE","value":"longitudinal"},{"schema":"INSPIRE","value":"CERN Lab"},{"schema":"INSPIRE","value":"acceptance"},{"schema":"INSPIRE","value":"transverse momentum dependence"},{"schema":"INSPIRE","value":"mass dependence"},{"schema":"INSPIRE","value":"Wilson"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"statistical analysis: Bayesian"},{"schema":"INSPIRE","value":"effective field theory"},{"schema":"INSPIRE","value":"topology"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2022-09-02T14:08:17","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-11T00:00:00","recid":132116,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},{"affiliation":"U. Oklahoma, Norman","full_name":"Abbott, B."},{"affiliation":"Massachusetts U., Amherst","full_name":"Abbott, D.C."},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, K."},{"affiliation":"Brookhaven","full_name":"Abidi, S.H."},{"affiliation":"Rabat U.","full_name":"Aboulhorma, A."},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, H."},{"affiliation":"Technion","full_name":"Abreu, H."},{"affiliation":"City Coll., N.Y.","full_name":"Abulaiti, Y."},{"affiliation":"Chile U., Catolica","full_name":"Abusleme Hoffman, A.C."}],"title":"Evidence for the charge asymmetry in $pp \\rightarrow t\\bar{t}$ production at $\\sqrt{s}= 13$ TeV with the ATLAS detector","total_tables":50,"type":["article"],"uuid":"ef710ef8-10fc-4ec7-992d-d9a4bfa78c18","version":1,"year":"2023"},{"abstract":"The LUX-ZEPLIN experiment is a dark matter detector centered on a dual-phase xenon time projection chamber operating at the Sanford Underground Research Facility in Lead, South Dakota, USA. This Letter reports results from LUX-ZEPLIN's first search for weakly interacting massive particles (WIMPs) with an exposure of 60~live days using a fiducial mass of 5.5 t. A profile-likelihood ratio analysis shows the data to be consistent with a background-only hypothesis, setting new limits on spin-independent WIMP-nucleon, spin-dependent WIMP-neutron, and spin-dependent WIMP-proton cross sections for WIMP masses above 9 GeV/c$^2$. The most stringent limit is set for spin-independent scattering at 36 GeV/c$^2$, rejecting cross sections above 9.2$\\times 10^{-48}$ cm$^2$ at the 90% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2107834/1/csv","json":"https://www.hepdata.net/download/submission/ins2107834/1/json","root":"https://www.hepdata.net/download/submission/ins2107834/1/root","yaml":"https://www.hepdata.net/download/submission/ins2107834/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2107834/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2207.03764","authors":["Aalbers, J.","Akerib, D.S.","Akerlof, C.W.","Musalhi, A.K. Al","Alder, F.","Alqahtani, A.","Alsum, S.K.","Amarasinghe, C.S.","Ames, A.","Anderson, T.J."],"collaborations":["LZ"],"control_number":"144760","creation_date":"2022-07-08","data":[{"abstract":"90% CL WIMP SI cross sections, including sensitivities","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2107834/SI cross section/csv","json":"https://www.hepdata.net/download/table/ins2107834/SI cross section/json","root":"https://www.hepdata.net/download/table/ins2107834/SI cross section/root","yaml":"https://www.hepdata.net/download/table/ins2107834/SI cross section/yaml","yoda":"https://www.hepdata.net/download/table/ins2107834/SI cross section/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145089","creation_date":"2022-07-08","data_keywords":{"cmenergies":[],"observables":["WIMP-nucleon cross section"],"phrases":["WIMP","spin-independent"],"reactions":["chi N-> chi N"]},"date":"08 Jul 2022","doc_type":"datatable","doi":"10.17182/hepdata.144760.v1/t1","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145089,"inspire_id":"2107834","journal_info":"Phys.Rev.Lett. 131 (2023) 041002","keywords":[{"name":"reactions","synonyms":"","value":"chi N-> chi N"},{"name":"observables","synonyms":"","value":"WIMP-nucleon cross section"},{"name":"phrases","synonyms":"","value":"WIMP"},{"name":"phrases","synonyms":"","value":"spin-independent"}],"last_updated":"2023-10-27T14:30:09","parent_child_join":{"name":"child_datatable","parent":"144760"},"recid":145089,"related_publication":144760,"title":"SI cross section","uuid":"b1364861-d142-4584-ab7b-9746fa641ae0"},{"abstract":"90% CL WIMP SDn cross sections, including sensitivities and nuclear structure uncertainties","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2107834/SDn cross section/csv","json":"https://www.hepdata.net/download/table/ins2107834/SDn cross section/json","root":"https://www.hepdata.net/download/table/ins2107834/SDn cross section/root","yaml":"https://www.hepdata.net/download/table/ins2107834/SDn cross section/yaml","yoda":"https://www.hepdata.net/download/table/ins2107834/SDn cross section/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145090","creation_date":"2022-07-08","data_keywords":{"cmenergies":[],"observables":["WIMP-neutron cross section"],"phrases":["spin-dependent-neutron","WIMP"],"reactions":["chi N-> chi N"]},"date":"08 Jul 2022","doc_type":"datatable","doi":"10.17182/hepdata.144760.v1/t2","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145090,"inspire_id":"2107834","journal_info":"Phys.Rev.Lett. 131 (2023) 041002","keywords":[{"name":"reactions","synonyms":"","value":"chi N-> chi N"},{"name":"observables","synonyms":"","value":"WIMP-neutron cross section"},{"name":"phrases","synonyms":"","value":"WIMP"},{"name":"phrases","synonyms":"","value":"spin-dependent-neutron"}],"last_updated":"2023-10-27T14:30:09","parent_child_join":{"name":"child_datatable","parent":"144760"},"recid":145090,"related_publication":144760,"title":"SDn cross section","uuid":"f90ad389-901e-479e-bd9a-5176e05a5773"},{"abstract":"90% CL WIMP SDp cross sections, including sensitivities and nuclear structure uncertainties","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2107834/SDp cross section/csv","json":"https://www.hepdata.net/download/table/ins2107834/SDp cross section/json","root":"https://www.hepdata.net/download/table/ins2107834/SDp cross section/root","yaml":"https://www.hepdata.net/download/table/ins2107834/SDp cross section/yaml","yoda":"https://www.hepdata.net/download/table/ins2107834/SDp cross section/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145091","creation_date":"2022-07-08","data_keywords":{"cmenergies":[],"observables":["WIMP-proton cross section"],"phrases":["WIMP","spin-dependent-protron"],"reactions":["chi N-> chi N"]},"date":"08 Jul 2022","doc_type":"datatable","doi":"10.17182/hepdata.144760.v1/t3","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145091,"inspire_id":"2107834","journal_info":"Phys.Rev.Lett. 131 (2023) 041002","keywords":[{"name":"reactions","synonyms":"","value":"chi N-> chi N"},{"name":"observables","synonyms":"","value":"WIMP-proton cross section"},{"name":"phrases","synonyms":"","value":"WIMP"},{"name":"phrases","synonyms":"","value":"spin-dependent-protron"}],"last_updated":"2023-10-27T14:30:09","parent_child_join":{"name":"child_datatable","parent":"144760"},"recid":145091,"related_publication":144760,"title":"SDp cross section","uuid":"81fa9043-e41f-4bac-8016-61f388ce71af"},{"abstract":"Data selection efficiency as a function of nuclear recoil energy","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2107834/Efficiency/csv","json":"https://www.hepdata.net/download/table/ins2107834/Efficiency/json","root":"https://www.hepdata.net/download/table/ins2107834/Efficiency/root","yaml":"https://www.hepdata.net/download/table/ins2107834/Efficiency/yaml","yoda":"https://www.hepdata.net/download/table/ins2107834/Efficiency/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145092","creation_date":"2022-07-08","data_keywords":{"cmenergies":[],"observables":["efficiency"],"phrases":["Xe nuclear recoil"]},"date":"08 Jul 2022","doc_type":"datatable","doi":"10.17182/hepdata.144760.v1/t4","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145092,"inspire_id":"2107834","journal_info":"Phys.Rev.Lett. 131 (2023) 041002","keywords":[{"name":"observables","synonyms":"","value":"efficiency"},{"name":"phrases","synonyms":"","value":"Xe nuclear recoil"}],"last_updated":"2023-10-27T14:30:09","parent_child_join":{"name":"child_datatable","parent":"144760"},"recid":145092,"related_publication":144760,"title":"Efficiency","uuid":"f96ce4e7-86fd-4b2c-8ff0-6f86ee11b4a1"},{"abstract":"Data points used in analysis in log_10(S2)-S1 space","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2107834/Data/csv","json":"https://www.hepdata.net/download/table/ins2107834/Data/json","root":"https://www.hepdata.net/download/table/ins2107834/Data/root","yaml":"https://www.hepdata.net/download/table/ins2107834/Data/yaml","yoda":"https://www.hepdata.net/download/table/ins2107834/Data/yoda"}},"authors":null,"collaborations":["LZ"],"control_number":"145093","creation_date":"2022-07-08","data_keywords":{"cmenergies":[],"observables":["log_10(S2)","S1"],"phrases":["data points","WIMP"]},"date":"08 Jul 2022","doc_type":"datatable","doi":"10.17182/hepdata.144760.v1/t5","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"id":145093,"inspire_id":"2107834","journal_info":"Phys.Rev.Lett. 131 (2023) 041002","keywords":[{"name":"observables","synonyms":"","value":"S1"},{"name":"observables","synonyms":"","value":"log_10(S2)"},{"name":"phrases","synonyms":"","value":"data points"},{"name":"phrases","synonyms":"","value":"WIMP"}],"last_updated":"2023-10-27T14:30:09","parent_child_join":{"name":"child_datatable","parent":"144760"},"recid":145093,"related_publication":144760,"title":"Data","uuid":"16d66051-fa44-4e88-a82f-8cdd160c5d33"}],"data_keywords":{"cmenergies":[],"observables":["efficiency","WIMP-neutron cross section","WIMP-nucleon cross section","S1","WIMP-proton cross section","log_10(S2)"],"phrases":["spin-dependent-neutron","spin-independent","Xe nuclear recoil","data points","WIMP","spin-dependent-protron"],"reactions":["chi N-> chi N"]},"date":"08 Jul 2022","doc_type":"publication","doi":"10.1103/PhysRevLett.131.041002","first_author":{"affiliation":"SLAC","full_name":"Aalbers, J."},"hepdata_doi":"10.17182/hepdata.144760","id":144760,"inspire_id":"2107834","journal_info":"Phys.Rev.Lett. 131 (2023) 041002","keywords":[{"schema":"INSPIRE","value":"dark matter: direct detection"},{"schema":"INSPIRE","value":"dark matter: detector"},{"schema":"INSPIRE","value":"WIMP: dark matter"},{"schema":"INSPIRE","value":"WIMP: mass"},{"schema":"INSPIRE","value":"time projection chamber: xenon"},{"schema":"INSPIRE","value":"WIMP nucleon: cross section"},{"schema":"INSPIRE","value":"WIMP p: cross section"},{"schema":"INSPIRE","value":"mass dependence"},{"schema":"INSPIRE","value":"spin: dependence"},{"schema":"INSPIRE","value":"channel cross section: upper limit"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"}],"last_updated":"2023-10-27T14:30:10","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-03-26T00:00:00","recid":144760,"subject_area":["Astrophysics","astro-ph.CO","hep-ex"],"summary_authors":[{"affiliation":"SLAC","full_name":"Aalbers, J."},{"affiliation":"SLAC","full_name":"Akerib, D.S."},{"affiliation":"Michigan U.","full_name":"Akerlof, C.W."},{"affiliation":"Oxford U.","full_name":"Musalhi, A.K. Al"},{"affiliation":"University Coll. London","full_name":"Alder, F."},{"affiliation":"Brown U. (main)","full_name":"Alqahtani, A."},{"affiliation":"Wisconsin U., Madison","full_name":"Alsum, S.K."},{"affiliation":"Michigan U.","full_name":"Amarasinghe, C.S."},{"affiliation":"SLAC","full_name":"Ames, A."},{"affiliation":"SLAC","full_name":"Anderson, T.J."}],"title":"First Dark Matter Search Results from the LUX-ZEPLIN (LZ) Experiment","total_tables":5,"type":["article"],"uuid":"237e8852-4eb9-4684-97a8-6aedc05a984a","version":1,"year":"2023"},{"abstract":"A combination of measurements of the inclusive top-quark pair production cross-section performed by ATLAS and CMS in proton-proton collisions at centre-of-mass energies of 7 and 8 TeV at the LHC is presented. The cross-sections are obtained using top-quark pair decays with an opposite-charge electron-muon pair in the final state and with data corresponding to an integrated luminosity of about 5 fb$^{-1}$ at $\\sqrt{s}=7$ TeV and about 20 fb$^{-1}$ at $\\sqrt{s}=8$ TeV for each experiment. The combined cross-sections are determined to be $178.5 \\pm 4.7$ pb at $\\sqrt{s}=7$ TeV and $243.3^{+6.0}_{-5.9}$ pb at $\\sqrt{s}=8$ TeV with a correlation of 0.41, using a reference top-quark mass value of 172.5 GeV. The ratio of the combined cross-sections is determined to be $R_{8/7}= 1.363\\pm 0.032$. The combined measured cross-sections and their ratio agree well with theory calculations using several parton distribution function (PDF) sets. The values of the top-quark pole mass (with the strong coupling fixed at 0.118) and the strong coupling (with the top-quark pole mass fixed at 172.5 GeV) are extracted from the combined results by fitting a next-to-next-to-leading-order plus next-to-next-to-leading-log QCD prediction to the measurements. Using a version of the NNPDF3.1 PDF set containing no top-quark measurements, the results obtained are $m_t^\\text{pole} = 173.4^{+1.8}_{-2.0}$ GeV and $\\alpha_\\text{s}(m_Z)= 0.1170^{+ 0.0021}_{-0.0018}$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2088291/1/csv","json":"https://www.hepdata.net/download/submission/ins2088291/1/json","root":"https://www.hepdata.net/download/submission/ins2088291/1/root","yaml":"https://www.hepdata.net/download/submission/ins2088291/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2088291/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2205.13830","authors":["Aad, G.","Abbott, B.","Abbott, D.C.","Abed Abud, A.","Abeling, K.","Abhayasinghe, D.K.","Abidi, S.H.","Aboulhorma, A.","Abramowicz, H.","Abreu, H."],"collaborations":["ATLAS","CMS"],"control_number":"110250","creation_date":"2022-05-27","data":[{"abstract":"Full covariance matrix including all systematic uncertainties expressed as nuisance parameters. \nWith the exception of the cross section parameters, all parameters were normalised to 1 before the fit. \nTherefore, the diagonal elements represent the constraint in quadrature.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2088291/CMS covariance matrix/csv","json":"https://www.hepdata.net/download/table/ins2088291/CMS covariance matrix/json","root":"https://www.hepdata.net/download/table/ins2088291/CMS covariance matrix/root","yaml":"https://www.hepdata.net/download/table/ins2088291/CMS covariance matrix/yaml","yoda":"https://www.hepdata.net/download/table/ins2088291/CMS covariance matrix/yoda"}},"authors":null,"collaborations":["ATLAS","CMS"],"control_number":"147192","creation_date":"2022-05-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0},{"gte":8000.0,"lte":8000.0}]},"date":"27 May 2022","doc_type":"datatable","doi":"10.17182/hepdata.110250.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":147192,"inspire_id":"2088291","journal_info":"JHEP 07 (2023) 213","keywords":[{"name":"cmenergies","synonyms":"","value":"7000"},{"name":"cmenergies","synonyms":"","value":"8000"}],"last_updated":"2024-02-08T19:54:32","parent_child_join":{"name":"child_datatable","parent":"110250"},"recid":147192,"related_publication":110250,"title":"CMS covariance matrix","uuid":"85f70199-1d6f-46c3-8a1b-0a65ccf12b28"},{"abstract":"Full covariance matrix including all systematic uncertainties expressed as nuisance parameters. \nWith the exception of the cross section parameters, all parameters were normalised to 1 before the fit. \nTherefore, the diagonal elements represent the constraint in quadrature.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2088291/Combination covariance matrix/csv","json":"https://www.hepdata.net/download/table/ins2088291/Combination covariance matrix/json","root":"https://www.hepdata.net/download/table/ins2088291/Combination covariance matrix/root","yaml":"https://www.hepdata.net/download/table/ins2088291/Combination covariance matrix/yaml","yoda":"https://www.hepdata.net/download/table/ins2088291/Combination covariance matrix/yoda"}},"authors":null,"collaborations":["ATLAS","CMS"],"control_number":"147193","creation_date":"2022-05-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0},{"gte":8000.0,"lte":8000.0}]},"date":"27 May 2022","doc_type":"datatable","doi":"10.17182/hepdata.110250.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":147193,"inspire_id":"2088291","journal_info":"JHEP 07 (2023) 213","keywords":[{"name":"cmenergies","synonyms":"","value":"7000"},{"name":"cmenergies","synonyms":"","value":"8000"}],"last_updated":"2024-02-08T19:54:32","parent_child_join":{"name":"child_datatable","parent":"110250"},"recid":147193,"related_publication":110250,"title":"Combination covariance matrix","uuid":"be4e4524-5f09-480f-949b-86862081d879"}],"data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0},{"gte":8000.0,"lte":8000.0}]},"date":"27 May 2022","doc_type":"publication","doi":"10.1007/JHEP07(2023)213","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"hepdata_doi":"10.17182/hepdata.110250","id":110250,"inspire_id":"2088291","journal_info":"JHEP 07 (2023) 213","keywords":[{"source":"author","value":"Hadron-Hadron Scattering"},{"source":"author","value":"Top Physics"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"top: pair production"},{"schema":"INSPIRE","value":"mass: pole"},{"schema":"INSPIRE","value":"parton: distribution function"},{"schema":"INSPIRE","value":"top: mass: measured"},{"schema":"INSPIRE","value":"channel cross section: measured"},{"schema":"INSPIRE","value":"perturbation theory: higher-order"},{"schema":"INSPIRE","value":"higher-order: 2"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"CMS"},{"schema":"INSPIRE","value":"strong coupling"},{"schema":"INSPIRE","value":"quantum chromodynamics: perturbation theory"},{"schema":"INSPIRE","value":"electron muon"},{"schema":"INSPIRE","value":"final state: ((n)jet dilepton)"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"correlation"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"7000 GeV-cms"},{"schema":"INSPIRE","value":"8000 GeV-cms"}],"last_updated":"2024-02-08T19:54:33","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-02-16T00:00:00","recid":110250,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},{"affiliation":"U. Oklahoma, Norman","full_name":"Abbott, B."},{"affiliation":"Massachusetts U., Amherst","full_name":"Abbott, D.C."},{"affiliation":"CERN","full_name":"Abed Abud, A."},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, K."},{"affiliation":"Royal Holloway, U. of London","full_name":"Abhayasinghe, D.K."},{"affiliation":"Brookhaven","full_name":"Abidi, S.H."},{"affiliation":"Rabat U.","full_name":"Aboulhorma, A."},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, H."},{"affiliation":"Technion","full_name":"Abreu, H."}],"title":"Combination of inclusive top-quark pair production cross-section measurements using ATLAS and CMS data at $\\sqrt{s}= 7$ and 8 TeV","total_tables":2,"type":["article"],"uuid":"f9e34003-d1ee-4508-9d97-3472ed834697","version":1,"year":"2023"},{"abstract":"We present a measurement of the $\\nu_e$-interaction rate in the MicroBooNE detector that addresses the observed MiniBooNE anomalous low-energy excess (LEE). The approach taken isolates neutrino interactions consistent with the kinematics of charged-current quasi-elastic (CCQE) events. The topology of such signal events has a final state with 1 electron, 1 proton, and 0 mesons ($1e1p$). Multiple novel techniques are employed to identify a $1e1p$ final state, including particle identification that use two methods of deep-learning-based image identification, and event isolation using a boosted decision-tree ensemble trained to recognize two-body scattering kinematics. This analysis selects 25 $\\nu_e$-candidate events in the reconstructed neutrino energy range of 200--1200 MeV, while $29.0 \\pm 1.9_\\text{(sys)} \\pm 5.4_\\text{(stat)}$ are predicted when using $\\nu_\\mu$ CCQE interactions as a constraint. We use a simplified model to translate the MiniBooNE LEE observation into a prediction for a $\\nu_e$ signal in MicroBooNE. A $\\Delta \\chi^2$ test statistic, based on the combined Neyman--Pearson $\\chi^2$ formalism, is used to define frequentist confidence intervals for the LEE signal strength. Using this technique, in the case of no LEE signal, we expect this analysis to exclude a normalization factor of 0.75 (0.98) times the median MiniBooNE LEE signal strength at 90% ($2\\sigma$) confidence level, while the MicroBooNE data yield an exclusion of 0.25 (0.38) times the median MiniBooNE LEE signal strength at 90% ($2\\sigma$) confidence","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1953568/1/csv","json":"https://www.hepdata.net/download/submission/ins1953568/1/json","root":"https://www.hepdata.net/download/submission/ins1953568/1/root","yaml":"https://www.hepdata.net/download/submission/ins1953568/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1953568/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2110.14080","authors":["Abratenko, P.","An, R.","Anthony, J.","Arellano, L.","Asaadi, J.","Ashkenazi, A.","Balasubramanian, S.","Baller, B.","Barnes, C.","Barr, G."],"collaborations":["MicroBooNE"],"control_number":"114859","creation_date":"2021-10-26","data":[{"abstract":"Observed NuE data and background (+ LEE) prediction, including the muon neutrino background prediction from the empirical fit, for arXiv:2110.14080. The prediction incorporates the constraint from the 1mu1p sample","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) constrained prediction/csv","json":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) constrained prediction/json","root":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) constrained prediction/root","yaml":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) constrained prediction/yaml","yoda":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) constrained prediction/yoda"}},"authors":null,"collaborations":["MicroBooNE"],"control_number":"114976","creation_date":"2021-10-26","data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"datatable","doi":"10.17182/hepdata.114859.v1/t1","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"id":114976,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"name":"reactions","synonyms":"","value":"NUE CCQE"},{"name":"observables","synonyms":"","value":"DN/DE"},{"name":"phrases","synonyms":"","value":"Neutrino LArTPC Interactions"}],"last_updated":"2021-11-08T15:57:32","parent_child_join":{"name":"child_datatable","parent":"114859"},"recid":114976,"related_publication":114859,"title":"NuE data and background (+ LEE) constrained prediction","uuid":"863df5d7-9360-41ea-8e5c-634b06c5993f"},{"abstract":"Observed NuE data and background (+ LEE) prediction, including the muon neutrino background prediction from the empirical fit, for arXiv:2110.14080. The prediction does not incorporate the constraint from the 1mu1p sample","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) unconstrained prediction/csv","json":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) unconstrained prediction/json","root":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) unconstrained prediction/root","yaml":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) unconstrained prediction/yaml","yoda":"https://www.hepdata.net/download/table/ins1953568/NuE data and background (+ LEE) unconstrained prediction/yoda"}},"authors":null,"collaborations":["MicroBooNE"],"control_number":"114977","creation_date":"2021-10-26","data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"datatable","doi":"10.17182/hepdata.114859.v1/t2","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"id":114977,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"name":"reactions","synonyms":"","value":"NUE CCQE"},{"name":"observables","synonyms":"","value":"DN/DE"},{"name":"phrases","synonyms":"","value":"Neutrino LArTPC Interactions"}],"last_updated":"2021-11-08T15:57:32","parent_child_join":{"name":"child_datatable","parent":"114859"},"recid":114977,"related_publication":114859,"title":"NuE data and background (+ LEE) unconstrained prediction","uuid":"2dc13f6d-9e68-423a-827b-ad4f6d21e6e5"},{"abstract":"NuE background fractional covariance matrix after the 1mu1p constraint from arXiv:2110.14080","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1953568/NuE background constrained fractional covariance matrix/csv","json":"https://www.hepdata.net/download/table/ins1953568/NuE background constrained fractional covariance matrix/json","root":"https://www.hepdata.net/download/table/ins1953568/NuE background constrained fractional covariance matrix/root","yaml":"https://www.hepdata.net/download/table/ins1953568/NuE background constrained fractional covariance matrix/yaml","yoda":"https://www.hepdata.net/download/table/ins1953568/NuE background constrained fractional covariance matrix/yoda"}},"authors":null,"collaborations":["MicroBooNE"],"control_number":"114978","creation_date":"2021-10-26","data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"datatable","doi":"10.17182/hepdata.114859.v1/t3","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"id":114978,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"name":"reactions","synonyms":"","value":"NUE CCQE"},{"name":"observables","synonyms":"","value":"DN/DE"},{"name":"phrases","synonyms":"","value":"Neutrino LArTPC Interactions"}],"last_updated":"2021-11-08T15:57:32","parent_child_join":{"name":"child_datatable","parent":"114859"},"recid":114978,"related_publication":114859,"title":"NuE background constrained fractional covariance matrix","uuid":"ac811aff-dc38-42b6-9957-34294d62cd59"},{"abstract":"NuE background+LEE fractional covariance matrix after the 1mu1p constraint from arXiv:2110.14080","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE constrained fractional covariance matrix/csv","json":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE constrained fractional covariance matrix/json","root":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE constrained fractional covariance matrix/root","yaml":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE constrained fractional covariance matrix/yaml","yoda":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE constrained fractional covariance matrix/yoda"}},"authors":null,"collaborations":["MicroBooNE"],"control_number":"114979","creation_date":"2021-10-26","data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"datatable","doi":"10.17182/hepdata.114859.v1/t4","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"id":114979,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"name":"reactions","synonyms":"","value":"NUE CCQE"},{"name":"observables","synonyms":"","value":"DN/DE"},{"name":"phrases","synonyms":"","value":"Neutrino LArTPC Interactions"}],"last_updated":"2021-11-08T15:57:32","parent_child_join":{"name":"child_datatable","parent":"114859"},"recid":114979,"related_publication":114859,"title":"NuE background+LEE constrained fractional covariance matrix","uuid":"cc2fb2bb-9e36-4bf3-bd63-05e77c1bf5d7"},{"abstract":"NuE background fractional covariance matrix before the 1mu1p constraint from arXiv:2110.14080","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1953568/NuE background unconstrained fractional covariance matrix/csv","json":"https://www.hepdata.net/download/table/ins1953568/NuE background unconstrained fractional covariance matrix/json","root":"https://www.hepdata.net/download/table/ins1953568/NuE background unconstrained fractional covariance matrix/root","yaml":"https://www.hepdata.net/download/table/ins1953568/NuE background unconstrained fractional covariance matrix/yaml","yoda":"https://www.hepdata.net/download/table/ins1953568/NuE background unconstrained fractional covariance matrix/yoda"}},"authors":null,"collaborations":["MicroBooNE"],"control_number":"114980","creation_date":"2021-10-26","data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"datatable","doi":"10.17182/hepdata.114859.v1/t5","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"id":114980,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"name":"reactions","synonyms":"","value":"NUE CCQE"},{"name":"observables","synonyms":"","value":"DN/DE"},{"name":"phrases","synonyms":"","value":"Neutrino LArTPC Interactions"}],"last_updated":"2021-11-08T15:57:32","parent_child_join":{"name":"child_datatable","parent":"114859"},"recid":114980,"related_publication":114859,"title":"NuE background unconstrained fractional covariance matrix","uuid":"c8e8f757-e2c1-4ff8-a30e-a6a2be248154"},{"abstract":"NuE background+LEE fractional covariance matrix before the 1mu1p constraint from arXiv:2110.14080","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE unconstrained fractional covariance matrix/csv","json":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE unconstrained fractional covariance matrix/json","root":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE unconstrained fractional covariance matrix/root","yaml":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE unconstrained fractional covariance matrix/yaml","yoda":"https://www.hepdata.net/download/table/ins1953568/NuE background+LEE unconstrained fractional covariance matrix/yoda"}},"authors":null,"collaborations":["MicroBooNE"],"control_number":"114981","creation_date":"2021-10-26","data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"datatable","doi":"10.17182/hepdata.114859.v1/t6","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"id":114981,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"name":"reactions","synonyms":"","value":"NUE CCQE"},{"name":"observables","synonyms":"","value":"DN/DE"},{"name":"phrases","synonyms":"","value":"Neutrino LArTPC Interactions"}],"last_updated":"2021-11-08T15:57:32","parent_child_join":{"name":"child_datatable","parent":"114859"},"recid":114981,"related_publication":114859,"title":"NuE background+LEE unconstrained fractional covariance matrix","uuid":"17359253-9905-4e7a-8879-b6d9c7672a2c"},{"abstract":"NuE simulation from arXiv:2110.14080","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1953568/NuE simulation/csv","json":"https://www.hepdata.net/download/table/ins1953568/NuE simulation/json","root":"https://www.hepdata.net/download/table/ins1953568/NuE simulation/root","yaml":"https://www.hepdata.net/download/table/ins1953568/NuE simulation/yaml","yoda":"https://www.hepdata.net/download/table/ins1953568/NuE simulation/yoda"}},"authors":null,"collaborations":["MicroBooNE"],"control_number":"114982","creation_date":"2021-10-26","data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"datatable","doi":"10.17182/hepdata.114859.v1/t7","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"id":114982,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"name":"reactions","synonyms":"","value":"NUE CCQE"},{"name":"observables","synonyms":"","value":"DN/DE"},{"name":"phrases","synonyms":"","value":"Neutrino LArTPC Interactions"}],"last_updated":"2021-11-08T15:57:32","parent_child_join":{"name":"child_datatable","parent":"114859"},"recid":114982,"related_publication":114859,"title":"NuE simulation","uuid":"15a5842b-e766-49d6-88ae-a060116d1e67"}],"data_keywords":{"cmenergies":[],"observables":["DN/DE"],"phrases":["Neutrino LArTPC Interactions"],"reactions":["NUE CCQE"]},"date":"26 Oct 2021","doc_type":"publication","doi":"10.1103/PhysRevD.105.112003","first_author":{"affiliation":"Tufts U.","full_name":"Abratenko, P."},"hepdata_doi":"10.17182/hepdata.114859","id":114859,"inspire_id":"1953568","journal_info":"Phys.Rev.D 105 (2022) 112003","keywords":[{"schema":"INSPIRE","value":"neutrino: interaction"},{"schema":"INSPIRE","value":"neutrino/e"},{"schema":"INSPIRE","value":"neutrino: energy"},{"schema":"INSPIRE","value":"BooNE"},{"schema":"INSPIRE","value":"charged current"},{"schema":"INSPIRE","value":"kinematics"},{"schema":"INSPIRE","value":"p: particle identification"},{"schema":"INSPIRE","value":"statistical analysis: frequentist"},{"schema":"INSPIRE","value":"electron: particle identification"},{"schema":"INSPIRE","value":"neutrino nucleus: inelastic scattering"},{"schema":"INSPIRE","value":"yield"},{"schema":"INSPIRE","value":"topology"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"}],"last_updated":"2021-11-08T15:57:34","parent_child_join":{"name":"parent_publication"},"publication_date":"2022-12-11T00:00:00","recid":114859,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Tufts U.","full_name":"Abratenko, P."},{"affiliation":"IIT, Chicago","full_name":"An, R."},{"affiliation":"Cambridge U.","full_name":"Anthony, J."},{"affiliation":"Manchester U.","full_name":"Arellano, L."},{"affiliation":"Texas U., Arlington","full_name":"Asaadi, J."},{"affiliation":"Tel Aviv U.","full_name":"Ashkenazi, A."},{"affiliation":"Fermilab","full_name":"Balasubramanian, S."},{"affiliation":"Fermilab","full_name":"Baller, B."},{"affiliation":"Michigan U.","full_name":"Barnes, C."},{"affiliation":"Oxford U.","full_name":"Barr, G."}],"title":"Search for an anomalous excess of charged-current quasi-elastic $\\nu_e$ interactions with the MicroBooNE experiment using Deep-Learning-based reconstruction","total_tables":7,"type":["article"],"uuid":"4be75cf7-c7fb-48f4-ba90-64590db8681e","version":1,"year":"2022"}],"total":444}