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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":"We determine the CKM matrix-element magnitude $|V_{cb}|$ using $\\overline{B}^0\\to D^{*+}\\ell^-\\bar\\nu_\\ell$ decays reconstructed in $189 \\, \\mathrm{fb}^{-1}$ of collision data collected by the Belle II experiment, located at the SuperKEKB $e^+e^-$ collider. Partial decay rates are reported as functions of the recoil parameter $w$ and three decay angles separately for electron and muon final states. We obtain $|V_{cb}|$ using the Boyd-Grinstein-Lebed and Caprini-Lellouch-Neubert parametrizations, and find $|V_{cb}|_\\mathrm{BGL}=(40.57\\pm 0.31 \\pm 0.95\\pm 0.58)\\times 10^{-3}$ and $|V_{cb}|_\\mathrm{CLN}=(40.13 \\pm 0.27 \\pm 0.93\\pm 0.58 )\\times 10^{-3}$ with the uncertainties denoting statistical components, systematic components, and components from the lattice QCD input, respectively. The branching fraction is measured to be ${\\cal B}(\\overline{B}^0\\to D^{*+}\\ell^-\\bar\\nu_\\ell)=(4.922 \\pm 0.023 \\pm 0.220)\\%$. The ratio of branching fractions for electron and muon final states is found to be $0.998 \\pm 0.009 \\pm 0.020$. In addition, we determine the forward-backward angular asymmetry and the $D^{*+}$ longitudinal polarization fractions. All results are compatible with lepton-flavor universality in the Standard Model.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2705370/1/csv","json":"https://www.hepdata.net/download/submission/ins2705370/1/json","root":"https://www.hepdata.net/download/submission/ins2705370/1/root","yaml":"https://www.hepdata.net/download/submission/ins2705370/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2705370/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2310.01170","authors":["Adachi, I.","Adamczyk, K.","Aggarwal, L.","Ahmed, H.","Aihara, H.","Akopov, N.","Aloisio, A.","Anh Ky, N.","Asner, D.M.","Atmacan, H."],"collaborations":["Belle-II"],"control_number":"145129","creation_date":"2023-10-02","data":[{"abstract":"Measured partial decay rates $\\Delta\\Gamma$ (in units of $10^{-15}$ GeV)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2705370/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2705370/Table 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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. 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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. 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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). 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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":"We present a measurement of the differential shapes of exclusive $B\\to D^* \\ell \\bar{\\nu}_\\ell$ ($B = B^-, \\bar{B}^0 $ and $\\ell = e, \\mu$) decays with hadronic tag-side reconstruction for the full Belle data set of $711\\,\\mathrm{fb}^{-1}$ integrated luminosity. We extract the Caprini-Lellouch-Neubert (CLN) and Boyd-Grinstein-Lebed (BGL) form factor parameters and use an external input for the absolute branching fractions to determine the Cabibbo-Kobayashi-Maskawa matrix element and find $|V_{cb}|_\\mathrm{CLN} = (40.1\\pm0.9)\\times 10^{-3}$ and $|V_{cb}|_\\mathrm{BGL} = (40.6\\pm 0.9)\\times 10^{-3}$ with the zero-recoil lattice QCD point $\\mathcal{F}(1) = 0.906 \\pm 0.013$. We also perform a study of the impact of preliminary beyond zero-recoil lattice QCD calculations on the $|V_{cb}|$ determinations. Additionally, we present the lepton flavor universality ratio $R_{e\\mu} = \\mathcal{B}(B \\to D^* e \\bar{\\nu}_e) / \\mathcal{B}(B \\to D^* \\mu \\bar{\\nu}_\\mu) = 0.990 \\pm 0.021 \\pm 0.023$, the electron and muon forward-backward asymmetry and their difference $\\Delta A_{FB}=0.022\\pm0.026\\pm 0.007$, and the electron and muon $D^*$ longitudinal polarization fraction and their difference $\\Delta F_L^{D^*} = 0.034 \\pm 0.024 \\pm 0.007$. The uncertainties quoted correspond to the statistical and systematic uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2624324/1/csv","json":"https://www.hepdata.net/download/submission/ins2624324/1/json","root":"https://www.hepdata.net/download/submission/ins2624324/1/root","yaml":"https://www.hepdata.net/download/submission/ins2624324/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2624324/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2301.07529","authors":["Prim, M.T.","Bernlochner, F.","Metzner, F.","Lieret, K.","Kuhr, T.","Adachi, I.","Aihara, H.","Al Said, S.","Asner, D.M.","Atmacan, H."],"collaborations":["Belle"],"control_number":"137767","creation_date":"2023-01-18","data":[{"abstract":"Bins used in the average spectrum (equivalent to the B0 case binning)","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/Binning Average/csv","json":"https://www.hepdata.net/download/table/ins2624324/Binning Average/json","root":"https://www.hepdata.net/download/table/ins2624324/Binning Average/root","yaml":"https://www.hepdata.net/download/table/ins2624324/Binning Average/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/Binning Average/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140425","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"observables":["DGAMMA/DX / GAMMA"],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t1","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140425,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"observables","synonyms":"","value":"DGAMMA/DX / GAMMA"},{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140425,"related_publication":137767,"title":"Binning Average","uuid":"7c3e96dc-6e10-4acc-bb21-e8ee9c975d9d"},{"abstract":"Bins for each data point for B0 and B+ cases separately.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/Binning Full/csv","json":"https://www.hepdata.net/download/table/ins2624324/Binning Full/json","root":"https://www.hepdata.net/download/table/ins2624324/Binning Full/root","yaml":"https://www.hepdata.net/download/table/ins2624324/Binning Full/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/Binning Full/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140426","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"observables":["DGAMMA/DX / GAMMA"],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t2","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140426,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"observables","synonyms":"","value":"DGAMMA/DX / GAMMA"},{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140426,"related_publication":137767,"title":"Binning Full","uuid":"5e871c25-68bb-4322-9670-4b8b57061a2c"},{"abstract":"The fully averaged measured shape.\nThe 40 entries correspond to 10 bins in w, cosThetaL, cosThetaV, and chi.\nFor the binning see the file 'Binning.yaml'.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrum/csv","json":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrum/json","root":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrum/root","yaml":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrum/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrum/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140427","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"observables":["DGAMMA/DX / GAMMA"],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t3","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140427,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"observables","synonyms":"","value":"DGAMMA/DX / GAMMA"},{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140427,"related_publication":137767,"title":"AverageSpectrum","uuid":"6888fa76-2a99-4097-81f1-b8ba9d844811"},{"abstract":"The full experimental statistical correlations for the averaged spectrum are shown. The index of the entry corresponds to the index of the corresponding central value.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumStatisticalCorrelation/csv","json":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumStatisticalCorrelation/json","root":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumStatisticalCorrelation/root","yaml":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumStatisticalCorrelation/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumStatisticalCorrelation/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140428","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t4","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140428,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140428,"related_publication":137767,"title":"AverageSpectrumStatisticalCorrelation","uuid":"1f73de07-ad9f-4984-a374-f0d2a562c63f"},{"abstract":"The full experimental systematic correlations for the averaged spectrum are shown. The index of the entry corresponds to the index of the corresponding central value.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumSystematicCorrelation/csv","json":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumSystematicCorrelation/json","root":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumSystematicCorrelation/root","yaml":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumSystematicCorrelation/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/AverageSpectrumSystematicCorrelation/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140429","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t5","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140429,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140429,"related_publication":137767,"title":"AverageSpectrumSystematicCorrelation","uuid":"4782cd5a-a0c2-484b-a957-56c545bf5fed"},{"abstract":"The individual measured shapes.\nThe 160 entries correspond to the 10 bins in w, cosThetaL, cosThetaV, and chi.\nIndex 0-40: B0 --> D* e nu\nIndex 40-80: B0 --> D* mu nu\nIndex 80-120: B+ --> D* e nu\nIndex 120-160: B+ --> D* mu nu\nFor the binning see the file 'Binning.yaml'.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectra/csv","json":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectra/json","root":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectra/root","yaml":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectra/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectra/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140430","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"observables":["DGAMMA/DX / GAMMA"],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t6","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140430,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"observables","synonyms":"","value":"DGAMMA/DX / GAMMA"},{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140430,"related_publication":137767,"title":"IndividualSpectra","uuid":"afc0b7c8-3e59-4ec6-8508-ae49ae06ffea"},{"abstract":"The full experimental statistical correlations for the individual spectra are shown. The index of the entry corresponds to the index of the corresponding central value.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraStatisticalCorrelation/csv","json":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraStatisticalCorrelation/json","root":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraStatisticalCorrelation/root","yaml":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraStatisticalCorrelation/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraStatisticalCorrelation/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140431","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t7","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140431,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140431,"related_publication":137767,"title":"IndividualSpectraStatisticalCorrelation","uuid":"30b01a1c-5692-4225-a06b-177ed9360028"},{"abstract":"The full experimental systematic correlations for the individual spectra are shown. The index of the entry corresponds to the index of the corresponding central value.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraSystematicCorrelation/csv","json":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraSystematicCorrelation/json","root":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraSystematicCorrelation/root","yaml":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraSystematicCorrelation/yaml","yoda":"https://www.hepdata.net/download/table/ins2624324/IndividualSpectraSystematicCorrelation/yoda"}},"authors":null,"collaborations":["Belle"],"control_number":"140432","creation_date":"2023-01-18","data_keywords":{"cmenergies":[],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.137767.v1/t8","first_author":{"affiliation":"","full_name":"Prim, M.T."},"id":140432,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"name":"reactions","synonyms":"","value":"B --> D* l+ nu_l"}],"last_updated":"2023-05-09T04:51:14","parent_child_join":{"name":"child_datatable","parent":"137767"},"recid":140432,"related_publication":137767,"title":"IndividualSpectraSystematicCorrelation","uuid":"51ec5b89-59bb-422e-acb2-87b18ccae181"}],"data_keywords":{"cmenergies":[],"observables":["DGAMMA/DX / GAMMA"],"reactions":["B --> D* l+ nu_l"]},"date":"18 Jan 2023","doc_type":"publication","doi":"10.1103/PhysRevD.108.012002","first_author":{"affiliation":"","full_name":"Prim, M.T."},"hepdata_doi":"10.17182/hepdata.137767","id":137767,"inspire_id":"2624324","journal_info":"Phys.Rev.D 108 (2023) 012002","keywords":[{"schema":"INSPIRE","value":"electron positron: annihilation"},{"schema":"INSPIRE","value":"electron positron: colliding beams"},{"schema":"INSPIRE","value":"B-: semileptonic decay"},{"schema":"INSPIRE","value":"anti-B0: semileptonic decay"},{"schema":"INSPIRE","value":"D*(2010)"},{"schema":"INSPIRE","value":"angular distribution: asymmetry"},{"schema":"INSPIRE","value":"lepton: flavor: universality"},{"schema":"INSPIRE","value":"polarization: longitudinal"},{"schema":"INSPIRE","value":"lattice field theory"},{"schema":"INSPIRE","value":"electron"},{"schema":"INSPIRE","value":"muon"},{"schema":"INSPIRE","value":"branching ratio: ratio: measured"},{"schema":"INSPIRE","value":"B-: branching ratio"},{"schema":"INSPIRE","value":"anti-B0: branching ratio"},{"schema":"INSPIRE","value":"production: asymmetry"},{"schema":"INSPIRE","value":"BELLE"},{"schema":"INSPIRE","value":"KEK-B"},{"schema":"INSPIRE","value":"error: statistical"},{"schema":"INSPIRE","value":"CKM matrix"},{"schema":"INSPIRE","value":"form factor"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"B --> D*(2010) electron neutrino/e"},{"schema":"INSPIRE","value":"B --> D*(2010) muon neutrino/mu"}],"last_updated":"2023-05-09T04:51:15","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-02-14T00:00:00","recid":137767,"subject_area":["hep-ex","Phenomenology-HEP","hep-ph"],"summary_authors":[{"affiliation":"","full_name":"Prim, M.T."},{"affiliation":"","full_name":"Bernlochner, F."},{"affiliation":"","full_name":"Metzner, F."},{"affiliation":"","full_name":"Lieret, K."},{"affiliation":"","full_name":"Kuhr, T."},{"affiliation":"","full_name":"Adachi, I."},{"affiliation":"","full_name":"Aihara, H."},{"affiliation":"","full_name":"Al Said, S."},{"affiliation":"","full_name":"Asner, D.M."},{"affiliation":"","full_name":"Atmacan, H."}],"title":"Measurement of Differential Distributions of $B \\to D^* \\ell \\bar \\nu_\\ell$ and Implications on $|V_{cb}|$","total_tables":8,"type":["article"],"uuid":"dc7faa0e-c43f-4653-b17e-3c519b743a22","version":1,"year":"2023"},{"abstract":"The $L_{\\mu}-L_{\\tau}$ extension of the standard model predicts the existence of a lepton-flavor-universality-violating $Z^{\\prime}$ boson that couples only to the heavier lepton families. We search for such a $Z^\\prime$ through its invisible decay in the process $e^+ e^- \\to \\mu^+ \\mu^- Z^{\\prime}$. We use a sample of electron-positron collisions at a center-of-mass energy of 10.58GeV collected by the Belle II experiment in 2019-2020, corresponding to an integrated luminosity of 79.7fb$^{-1}$. We find no excess over the expected standard-model background. We set 90$\\%$-confidence-level upper limits on the cross section for this process as well as on the coupling of the model, which ranges from $3 \\times 10^{-3}$ at low $Z^{\\prime}$ masses to 1 at $Z^{\\prime}$ masses of 8$GeV/c^{2}$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2611344/1/csv","json":"https://www.hepdata.net/download/submission/ins2611344/1/json","root":"https://www.hepdata.net/download/submission/ins2611344/1/root","yaml":"https://www.hepdata.net/download/submission/ins2611344/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2611344/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2212.03066","authors":["Adachi, I.","Adamczyk, K.","Aggarwal, L.","Ahmed, H.","Aihara, H.","Akopov, N.","Aloisio, A.","Anh Ky, N.","Asner, D.M.","Aushev, T."],"collaborations":["Belle-II"],"control_number":"138160","creation_date":"2022-12-06","data":[{"abstract":"Observed 90% CL upper limits on the cross section $\\sigma (e^+ e^- \\to \\mu^+ \\mu^- Z', Z' \\to $ invisible) as functions of the $Z'$ mass for the cases of negligible $\\Gamma_{Z'}$ and for $\\Gamma_{Z'} = 0.1 M_{Z'}$. Also shown are previous limits from Belle II.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2611344/Fig. 2 (bottom right)/csv","json":"https://www.hepdata.net/download/table/ins2611344/Fig. 2 (bottom right)/json","root":"https://www.hepdata.net/download/table/ins2611344/Fig. 2 (bottom right)/root","yaml":"https://www.hepdata.net/download/table/ins2611344/Fig. 2 (bottom right)/yaml","yoda":"https://www.hepdata.net/download/table/ins2611344/Fig. 2 (bottom right)/yoda"}},"authors":null,"collaborations":["Belle-II"],"control_number":"145901","creation_date":"2022-12-06","data_keywords":{"cmenergies":[],"observables":["Cross section"]},"date":"06 Dec 2022","doc_type":"datatable","doi":"10.17182/hepdata.138160.v1/t1","first_author":{"affiliation":"","full_name":"Adachi, I."},"id":145901,"inspire_id":"2611344","journal_info":"Phys.Rev.Lett. 130 (2023) 231801","keywords":[{"name":"observables","synonyms":"","value":"Cross section"}],"last_updated":"2023-12-13T17:05:46","parent_child_join":{"name":"child_datatable","parent":"138160"},"recid":145901,"related_publication":138160,"title":"Fig. 2 (bottom right)","uuid":"5b595edf-cc06-4805-bb48-1f57a6f3f319"},{"abstract":"Observed 90% CL upper limits on the coupling $g'$ for the fully invisible $L_\\mu \u2212 L_\\tau$ model as functions of the $Z'$ mass for the cases of negligible $\\Gamma_{Z'}$ and for $\\Gamma_{Z'} = 0.1 M_{Z'}$. Also shown are previous limits from NA64-e and Belle II searches. The red band shows the region that explains the muon anomalous magnetic moment $(g - 2)_\\mu \\pm 2 \\sigma$. The vertical dashed line indicates the limit beyond which the hypothesis $B(Z' \\to \\chi\\bar{\\chi}) \\approx 1$ is not respected in the negligible $\\Gamma_{Z'}$ case.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2611344/Fig. 3 (top left)/csv","json":"https://www.hepdata.net/download/table/ins2611344/Fig. 3 (top left)/json","root":"https://www.hepdata.net/download/table/ins2611344/Fig. 3 (top left)/root","yaml":"https://www.hepdata.net/download/table/ins2611344/Fig. 3 (top left)/yaml","yoda":"https://www.hepdata.net/download/table/ins2611344/Fig. 3 (top left)/yoda"}},"authors":null,"collaborations":["Belle-II"],"control_number":"145902","creation_date":"2022-12-06","data_keywords":{"cmenergies":[],"observables":["Coupling g', fully invisible model"]},"date":"06 Dec 2022","doc_type":"datatable","doi":"10.17182/hepdata.138160.v1/t2","first_author":{"affiliation":"","full_name":"Adachi, I."},"id":145902,"inspire_id":"2611344","journal_info":"Phys.Rev.Lett. 130 (2023) 231801","keywords":[{"name":"observables","synonyms":"","value":"Coupling g', fully invisible model"}],"last_updated":"2023-12-13T17:05:46","parent_child_join":{"name":"child_datatable","parent":"138160"},"recid":145902,"related_publication":138160,"title":"Fig. 3 (top left)","uuid":"2b71d8a1-7fb5-48da-9234-f23230aaa337"},{"abstract":"Observed 90% CL upper limits on the coupling $g'$ for the vanilla $L_\\mu \u2212 L_\\tau$ model as functions of the $Z'$ mass. Also shown are previous limits from Belle II and NA64-e searches for invisible $Z'$ decays, and from Belle, BaBar and CMS searches for $Z'$ decays to muons (at 95% CL). The red band shows the region that explains the muon anomalous magnetic moment $(g - 2)_\\mu \\pm 2 \\sigma$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2611344/Fig. 4 (middle left)/csv","json":"https://www.hepdata.net/download/table/ins2611344/Fig. 4 (middle left)/json","root":"https://www.hepdata.net/download/table/ins2611344/Fig. 4 (middle left)/root","yaml":"https://www.hepdata.net/download/table/ins2611344/Fig. 4 (middle left)/yaml","yoda":"https://www.hepdata.net/download/table/ins2611344/Fig. 4 (middle left)/yoda"}},"authors":null,"collaborations":["Belle-II"],"control_number":"145903","creation_date":"2022-12-06","data_keywords":{"cmenergies":[],"observables":["Coupling g', vanilla model"]},"date":"06 Dec 2022","doc_type":"datatable","doi":"10.17182/hepdata.138160.v1/t3","first_author":{"affiliation":"","full_name":"Adachi, I."},"id":145903,"inspire_id":"2611344","journal_info":"Phys.Rev.Lett. 130 (2023) 231801","keywords":[{"name":"observables","synonyms":"","value":"Coupling g', vanilla model"}],"last_updated":"2023-12-13T17:05:46","parent_child_join":{"name":"child_datatable","parent":"138160"},"recid":145903,"related_publication":138160,"title":"Fig. 4 (middle left)","uuid":"51282979-1027-4fd7-b553-398f6ecf5895"},{"abstract":"Best fit of the cross section.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2611344/No figure/csv","json":"https://www.hepdata.net/download/table/ins2611344/No figure/json","root":"https://www.hepdata.net/download/table/ins2611344/No figure/root","yaml":"https://www.hepdata.net/download/table/ins2611344/No figure/yaml","yoda":"https://www.hepdata.net/download/table/ins2611344/No figure/yoda"}},"authors":null,"collaborations":["Belle-II"],"control_number":"145904","creation_date":"2022-12-06","data_keywords":{"cmenergies":[],"observables":["best fit cross section"]},"date":"06 Dec 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dependence"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"electron positron --> muon+ muon- Z'"},{"schema":"INSPIRE","value":"10.58 GeV-cms"}],"last_updated":"2023-12-13T17:05:47","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-13T00:00:00","recid":138160,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"","full_name":"Adachi, I."},{"affiliation":"","full_name":"Adamczyk, K."},{"affiliation":"","full_name":"Aggarwal, L."},{"affiliation":"","full_name":"Ahmed, H."},{"affiliation":"","full_name":"Aihara, H."},{"affiliation":"","full_name":"Akopov, N."},{"affiliation":"","full_name":"Aloisio, A."},{"affiliation":"","full_name":"Anh Ky, N."},{"affiliation":"","full_name":"Asner, D.M."},{"affiliation":"","full_name":"Aushev, T."}],"title":"Search for an invisible $Z^\\prime$ in a final state with two muons and missing energy at Belle II","total_tables":4,"type":["article"],"uuid":"33e66782-dc52-453e-9c25-3eef524b8bb8","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. 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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. 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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"}],"total":685}