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TeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2628969/Table 9/csv","json":"https://www.hepdata.net/download/table/ins2628969/Table 9/json","root":"https://www.hepdata.net/download/table/ins2628969/Table 9/root","yaml":"https://www.hepdata.net/download/table/ins2628969/Table 9/yaml","yoda":"https://www.hepdata.net/download/table/ins2628969/Table 9/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"141086","creation_date":"2023-02-02","data_keywords":{"cmenergies":[{"gte":2760.0,"lte":2760.0}],"observables":["SPC"],"reactions":["PB PB --> CHARGED X"]},"date":"02 Feb 2023","doc_type":"datatable","doi":"10.17182/hepdata.141027.v1/t9","first_author":{},"id":141086,"inspire_id":"2628969","journal_info":"Eur.Phys.J.C 83 (2023) 576","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED 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Phys. Inst.","full_name":"Adamov\u00e1, D."},{"affiliation":"Frankfurt U.","full_name":"Adler, A."},{"affiliation":"CERN","full_name":"Aglieri Rinella, G."},{"affiliation":"INFN, Turin","full_name":"Agnello, M."},{"affiliation":"INFN, Bologna","full_name":"Agrawal, N."},{"affiliation":"Calcutta, VECC","full_name":"Ahammed, Z."},{"affiliation":"Aligarh Muslim U.","full_name":"Ahmad, S."},{"affiliation":"KISTI, Daejeon","full_name":"Ahn, S.U."},{"affiliation":"Kosice U.","full_name":"Ahuja, I."}],"title":"Symmetry plane correlations in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$TeV","total_tables":9,"type":["article"],"uuid":"b965496e-5a30-4435-84fe-4170043127e1","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). 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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. 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. 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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 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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, 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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":"The first measurement of the ${\\rm e}^{+}{\\rm e}^{-}$ pair production at low lepton pair transverse momentum ($p_{\\rm T,ee}$) and low invariant mass ($m_{\\rm ee}$) in non-central Pb$-$Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV at the LHC is presented. The dielectron production is studied with the ALICE detector at midrapidity ($|\\eta_{\\rm e}| < 0.8$) as a function of invariant mass ($0.4 \\leq m_{\\rm ee} < 2.7$ GeV/$c^2$) in the 50$-$70% and 70$-$90% centrality classes for $p_{\\rm T,ee} < 0.1$ GeV/$c$, and as a function of $p_{\\rm T,ee}$ in three $m_{\\rm ee}$ intervals in the most peripheral Pb$-$Pb collisions. Below a $p_{\\rm T,ee}$ of 0.1 GeV/$c$, a clear excess of ${\\rm e}^{+}{\\rm e}^{-}$ pairs is found compared to the expectations from known hadronic sources and predictions of thermal radiation from the medium. The $m_{\\rm ee}$ excess spectra are reproduced, within uncertainties, by different predictions of the photon$-$photon production of dielectrons, where the photons originate from the extremely strong electromagnetic fields generated by the highly Lorentz-contracted Pb nuclei. Lowest-order quantum electrodynamic (QED) calculations, as well as a model that takes into account the impact-parameter dependence of the average transverse momentum of the photons, also provide a good description of the $p_{\\rm T,ee}$ spectra. The measured $\\sqrt{\\langle p_{\\rm T,ee}^{2} \\rangle}$ of the excess $p_{\\rm T,ee}$ spectrum in peripheral Pb$-$Pb collisions is found to be comparable to the values observed previously at RHIC in a similar phase-space region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2071861/1/csv","json":"https://www.hepdata.net/download/submission/ins2071861/1/json","root":"https://www.hepdata.net/download/submission/ins2071861/1/root","yaml":"https://www.hepdata.net/download/submission/ins2071861/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2071861/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2204.11732","authors":["Acharya, S.","Adamov\u00e1, D.","Adler, A.","Aglieri Rinella, G.","Agnello, M.","Agrawal, N.","Ahammed, Z.","Ahmad, S.","Ahn, S.U.","Ahuja, I."],"collaborations":["ALICE"],"control_number":"134246","creation_date":"2022-04-25","data":[{"abstract":"Differential $e^+e^-$ yield in 50--70\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $m_{\\rm ee}$ for $p_{\\rm T,ee} < 0.1$ GeV/$c$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 1/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 1/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134483","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dM"],"phrases":["Dielectron yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t1","first_author":{},"id":134483,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dM"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134483,"related_publication":134246,"title":"Table 1","uuid":"5effba98-27a7-4e01-9f73-065f747cc61c"},{"abstract":"Differential $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $m_{\\rm ee}$ for $p_{\\rm T,ee} < 0.1$ GeV/$c$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 2/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 2/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134484","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dM"],"phrases":["Dielectron yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t2","first_author":{},"id":134484,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dM"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134484,"related_publication":134246,"title":"Table 2","uuid":"ffed2114-c3e8-4ea5-91fd-691483b7978e"},{"abstract":"Differential excess $e^+e^-$ yield in 50--70\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $m_{\\rm ee}$ for $p_{\\rm T,ee} < 0.1$ GeV/$c$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 3/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 3/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 3/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134485","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dM"],"phrases":["Dielectron excess yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t3","first_author":{},"id":134485,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dM"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron excess yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134485,"related_publication":134246,"title":"Table 3","uuid":"6996781d-ad9c-4f45-9ee4-c4fc54890d8f"},{"abstract":"Differential excess $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $m_{\\rm ee}$ for $p_{\\rm T,ee} < 0.1$ GeV/$c$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 4/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 4/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 4/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134486","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dM"],"phrases":["Dielectron excess yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t4","first_author":{},"id":134486,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dM"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron excess yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134486,"related_publication":134246,"title":"Table 4","uuid":"c893be29-356f-479b-9285-ffc4b08f418e"},{"abstract":"Differential $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $p_{\\rm T,ee}$ for 0.4 $< m_{\\rm ee} < 0.7$ GeV/$c^{\\rm 2}$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 5/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 5/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 5/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134487","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dPTEE"],"phrases":["Dielectron yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t5","first_author":{},"id":134487,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dPTEE"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134487,"related_publication":134246,"title":"Table 5","uuid":"9e65abe5-7bf1-46ae-a3b6-7af8d8a8563a"},{"abstract":"Differential $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $p_{\\rm T,ee}$ for 0.7 $< m_{\\rm ee} < 1.1$ GeV/$c^{\\rm 2}$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 6/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 6/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 6/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 6/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 6/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134488","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dPTEE"],"phrases":["Dielectron yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t6","first_author":{},"id":134488,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dPTEE"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134488,"related_publication":134246,"title":"Table 6","uuid":"066173dd-fa98-4d21-984b-e2dfd967844e"},{"abstract":"Differential $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $p_{\\rm T,ee}$ for 1.1 $< m_{\\rm ee} < 2.7$ GeV/$c^{\\rm 2}$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 7/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 7/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 7/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 7/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 7/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134489","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dPTEE"],"phrases":["Dielectron yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t7","first_author":{},"id":134489,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dPTEE"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134489,"related_publication":134246,"title":"Table 7","uuid":"7e6bd063-ca16-44bc-960b-a63bfe160564"},{"abstract":"Differential excess $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $p^{2}_{\\rm T,ee}$ for 0.4 $< m_{\\rm ee} < 0.7$ GeV/$c^{\\rm 2}$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 8/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 8/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 8/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 8/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 8/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134490","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dPTEE**2"],"phrases":["Dielectron excess yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t8","first_author":{},"id":134490,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dPTEE**2"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron excess yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134490,"related_publication":134246,"title":"Table 8","uuid":"db655903-0732-420c-ba51-3ddeee9f1a5a"},{"abstract":"Differential excess $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $p^{2}_{\\rm T,ee}$ for 0.7 $< m_{\\rm ee} < 1.1$ GeV/$c^{\\rm 2}$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$. The quoted upper limits correspond to a 90% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 9/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 9/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 9/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 9/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 9/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134491","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dPTEE**2"],"phrases":["Dielectron excess yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t9","first_author":{},"id":134491,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dPTEE**2"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron excess yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134491,"related_publication":134246,"title":"Table 9","uuid":"09fdef86-9e81-412a-95d2-5c7ea4221ec2"},{"abstract":"Differential excess $e^+e^-$ yield in 70--90\\% Pb--Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV as a function of $p^{2}_{\\rm T,ee}$ for 1.1 $< m_{\\rm ee} < 2.7$ GeV/$c^{\\rm 2}$. Electrons are measured within $|\\eta_{\\rm e}| < 0.8$ and $p_{\\rm T,e} > 0.2$ GeV/$c$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071861/Table 10/csv","json":"https://www.hepdata.net/download/table/ins2071861/Table 10/json","root":"https://www.hepdata.net/download/table/ins2071861/Table 10/root","yaml":"https://www.hepdata.net/download/table/ins2071861/Table 10/yaml","yoda":"https://www.hepdata.net/download/table/ins2071861/Table 10/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"134492","creation_date":"2022-04-25","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dPTEE**2"],"phrases":["Dielectron excess yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.134246.v1/t10","first_author":{},"id":134492,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> E+ E- X"},{"name":"observables","synonyms":"","value":"1/Nevt* dN/dPTEE**2"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"phrases","synonyms":"","value":"Dielectron excess yield"}],"last_updated":"2022-10-17T07:51:21","parent_child_join":{"name":"child_datatable","parent":"134246"},"recid":134492,"related_publication":134246,"title":"Table 10","uuid":"277a85b5-f16d-41f3-a3f1-82a924b8c136"}],"data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["1/Nevt* dN/dPTEE**2","1/Nevt* dN/dM","1/Nevt* dN/dPTEE"],"phrases":["Dielectron yield","Dielectron excess yield"],"reactions":["PB PB --> E+ E- X"]},"date":"25 Apr 2022","doc_type":"publication","doi":"10.1007/JHEP06(2023)024","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},"hepdata_doi":"10.17182/hepdata.134246","id":134246,"inspire_id":"2071861","journal_info":"JHEP 06 (2023) 024","keywords":[{"source":"author","value":"Jets and Jet Substructure"},{"source":"author","value":"Quark-Gluon Plasma"},{"schema":"INSPIRE","value":"dilepton: production"},{"schema":"INSPIRE","value":"electromagnetic field: high"},{"schema":"INSPIRE","value":"photon: transverse momentum"},{"schema":"INSPIRE","value":"radiation: thermal"},{"schema":"INSPIRE","value":"photon: production"},{"schema":"INSPIRE","value":"transverse momentum: low"},{"schema":"INSPIRE","value":"impact parameter: dependence"},{"schema":"INSPIRE","value":"peripheral"},{"schema":"INSPIRE","value":"pair production"},{"schema":"INSPIRE","value":"quantum electrodynamics"},{"schema":"INSPIRE","value":"ALICE"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"Brookhaven RHIC Coll"},{"schema":"INSPIRE","value":"phase space"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"5020 GeV-cms/nucleon "}],"last_updated":"2022-10-17T07:51:23","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-02-14T00:00:00","recid":134246,"subject_area":["nucl-ex","hep-ex"],"summary_authors":[{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},{"affiliation":"Rez, Nucl. Phys. Inst.","full_name":"Adamov\u00e1, D."},{"affiliation":"Frankfurt U.","full_name":"Adler, A."},{"affiliation":"CERN","full_name":"Aglieri Rinella, G."},{"affiliation":"INFN, Turin","full_name":"Agnello, M."},{"affiliation":"INFN, Bologna","full_name":"Agrawal, N."},{"affiliation":"Calcutta, VECC","full_name":"Ahammed, Z."},{"affiliation":"Aligarh Muslim U.","full_name":"Ahmad, S."},{"affiliation":"KISTI, Daejeon","full_name":"Ahn, S.U."},{"affiliation":"Kosice U.","full_name":"Ahuja, I."}],"title":"Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb$-$Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV","total_tables":10,"type":["article"],"uuid":"1ea22c00-e8d6-4444-93bc-a58dc089c5eb","version":1,"year":"2023"},{"abstract":"The first measurement of event-by-event antideuteron number fluctuations in high energy heavy-ion collisions is presented. The measurements are carried out at midrapidity ($|\\eta| < 0.8$) as a function of collision centrality in Pb$-$Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV using the ALICE detector. A significant negative correlation between the produced antiprotons and antideuterons is observed in all collision centralities. The results are compared with coalescence calculations, which fail to describe the measurement, in particular if a correlated production of protons and neutrons is assumed. Thermal-statistical model calculations describe the data within uncertainties only for correlation volumes that are different with respect to those describing proton yields and a similar measurement of net-proton number fluctuations.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2070391/1/csv","json":"https://www.hepdata.net/download/submission/ins2070391/1/json","root":"https://www.hepdata.net/download/submission/ins2070391/1/root","yaml":"https://www.hepdata.net/download/submission/ins2070391/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2070391/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2204.10166","authors":["Acharya, S.","Adamov\u00e1, D.","Adler, A.","Aglieri Rinella, G.","Agnello, M.","Agrawal, N.","Ahammed, Z.","Ahmad, S.","Ahn, S.U.","Ahuja, I."],"collaborations":["ALICE"],"control_number":"136310","creation_date":"2022-04-21","data":[{"abstract":"Second order to first order cumulant ratio of the $\\overline{d}$ multiplicity distribution as a function of collision centrality in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2070391/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2070391/Table 1/json","root":"https://www.hepdata.net/download/table/ins2070391/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2070391/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2070391/Table 1/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"144173","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["kappa2/kappa1"],"reactions":["Pb Pb --> $\\overline{d}$ + $X$"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.136310.v1/t1","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},"id":144173,"inspire_id":"2070391","journal_info":"Phys.Rev.Lett. 131 (2023) 041901","keywords":[{"name":"observables","synonyms":"","value":"kappa2/kappa1"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"reactions","synonyms":"","value":"Pb Pb --> $\\overline{d}$ + $X$"}],"last_updated":"2023-09-07T09:17:40","parent_child_join":{"name":"child_datatable","parent":"136310"},"recid":144173,"related_publication":136310,"title":"Table 1","uuid":"3c87d9a7-2ecf-4e73-96de-a8a04759b305"},{"abstract":"Pearson correlation between the measured $\\overline{p}$ and $\\overline{d}$ as a function of collision centrality in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2070391/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2070391/Table 2/json","root":"https://www.hepdata.net/download/table/ins2070391/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2070391/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2070391/Table 2/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"144174","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["rho"],"reactions":["Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.136310.v1/t2","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},"id":144174,"inspire_id":"2070391","journal_info":"Phys.Rev.Lett. 131 (2023) 041901","keywords":[{"name":"observables","synonyms":"","value":"rho"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"reactions","synonyms":"","value":"Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"}],"last_updated":"2023-09-07T09:17:40","parent_child_join":{"name":"child_datatable","parent":"136310"},"recid":144174,"related_publication":136310,"title":"Table 2","uuid":"6bba6c76-10b0-402b-a231-c306e2357496"},{"abstract":"Dependence of $\\overline{p}$-$\\overline{d}$ correlation on pseudorapidity acceptance of $\\overline{p}$ and $\\overline{d}$ selection in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV. Results are for 0.0--10.0$\\%$ collision centrality.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2070391/Table 3/csv","json":"https://www.hepdata.net/download/table/ins2070391/Table 3/json","root":"https://www.hepdata.net/download/table/ins2070391/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins2070391/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2070391/Table 3/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"144175","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["rho"],"reactions":["Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.136310.v1/t3","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},"id":144175,"inspire_id":"2070391","journal_info":"Phys.Rev.Lett. 131 (2023) 041901","keywords":[{"name":"observables","synonyms":"","value":"rho"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"reactions","synonyms":"","value":"Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"}],"last_updated":"2023-09-07T09:17:40","parent_child_join":{"name":"child_datatable","parent":"136310"},"recid":144175,"related_publication":136310,"title":"Table 3","uuid":"8cee17ec-47b2-4f7b-80d4-269d77adb9a6"},{"abstract":"Dependence of $\\overline{p}$-$\\overline{d}$ correlation on pseudorapidity acceptance of $\\overline{p}$ and $\\overline{d}$ selection in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV. Results are for 20.0--30.0$\\%$ collision centrality.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2070391/Table 4/csv","json":"https://www.hepdata.net/download/table/ins2070391/Table 4/json","root":"https://www.hepdata.net/download/table/ins2070391/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins2070391/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2070391/Table 4/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"144176","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["rho"],"reactions":["Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.136310.v1/t4","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},"id":144176,"inspire_id":"2070391","journal_info":"Phys.Rev.Lett. 131 (2023) 041901","keywords":[{"name":"observables","synonyms":"","value":"rho"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"reactions","synonyms":"","value":"Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"}],"last_updated":"2023-09-07T09:17:40","parent_child_join":{"name":"child_datatable","parent":"136310"},"recid":144176,"related_publication":136310,"title":"Table 4","uuid":"b9eb0e27-4410-4b79-8fb5-50403476cea1"},{"abstract":"Dependence of $\\overline{p}$-$\\overline{d}$ correlation on pseudorapidity acceptance of $\\overline{p}$ and $\\overline{d}$ selection in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV. Results are for 50.0--60.0$\\%$ collision centrality.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2070391/Table 5/csv","json":"https://www.hepdata.net/download/table/ins2070391/Table 5/json","root":"https://www.hepdata.net/download/table/ins2070391/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins2070391/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins2070391/Table 5/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"144177","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["rho"],"reactions":["Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.136310.v1/t5","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},"id":144177,"inspire_id":"2070391","journal_info":"Phys.Rev.Lett. 131 (2023) 041901","keywords":[{"name":"observables","synonyms":"","value":"rho"},{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"reactions","synonyms":"","value":"Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$"}],"last_updated":"2023-09-07T09:17:40","parent_child_join":{"name":"child_datatable","parent":"136310"},"recid":144177,"related_publication":136310,"title":"Table 5","uuid":"05f5a0c1-57e7-4855-b117-b78a2877fcc7"}],"data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["kappa2/kappa1","rho"],"reactions":["Pb Pb --> $\\overline{p}$ + $X$, $\\overline{d}$ + $X$","Pb Pb --> $\\overline{d}$ + $X$"]},"date":"21 Apr 2022","doc_type":"publication","doi":"10.1103/PhysRevLett.131.041901","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},"hepdata_doi":"10.17182/hepdata.136310","id":136310,"inspire_id":"2070391","journal_info":"Phys.Rev.Lett. 131 (2023) 041901","keywords":[{"schema":"INSPIRE","source":"classifier","value":"heavy ion, scattering"},{"schema":"INSPIRE","source":"classifier","value":"energy, high"},{"schema":"INSPIRE","source":"classifier","value":"heavy ion, energy"},{"schema":"INSPIRE","source":"classifier","value":"antideuteron, production"},{"schema":"INSPIRE","source":"classifier","value":"p, yield"},{"schema":"INSPIRE","source":"classifier","value":"fluctuation"},{"schema":"INSPIRE","value":"particle number: fluctuation"},{"schema":"INSPIRE","value":"energy: high"},{"schema":"INSPIRE","value":"p: production"},{"schema":"INSPIRE","value":"heavy ion: scattering"},{"schema":"INSPIRE","value":"p: yield"},{"schema":"INSPIRE","value":"antideuteron"},{"schema":"INSPIRE","source":"classifier","value":"correlation"},{"schema":"INSPIRE","source":"classifier","value":"anti-p"},{"schema":"INSPIRE","source":"classifier","value":"higher-order"},{"schema":"INSPIRE","source":"classifier","value":"coalescence"},{"schema":"INSPIRE","source":"classifier","value":"ALICE"},{"schema":"INSPIRE","source":"classifier","value":"multiplicity"},{"schema":"INSPIRE","source":"classifier","value":"CERN LHC Coll"},{"schema":"INSPIRE","source":"classifier","value":"TeV"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"5020 GeV-cms/nucleon "}],"last_updated":"2023-09-07T09:17:41","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-11T00:00:00","recid":136310,"subject_area":["nucl-ex","hep-ex"],"summary_authors":[{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, S."},{"affiliation":"Rez, Nucl. Phys. Inst.","full_name":"Adamov\u00e1, D."},{"affiliation":"Frankfurt U.","full_name":"Adler, A."},{"affiliation":"CERN","full_name":"Aglieri Rinella, G."},{"affiliation":"INFN, Turin","full_name":"Agnello, M."},{"affiliation":"INFN, Bologna","full_name":"Agrawal, N."},{"affiliation":"Calcutta, VECC","full_name":"Ahammed, Z."},{"affiliation":"Aligarh Muslim U.","full_name":"Ahmad, S."},{"affiliation":"KISTI, Daejeon","full_name":"Ahn, S.U."},{"affiliation":"Kosice U.","full_name":"Ahuja, I."}],"title":"First measurement of antideuteron number fluctuations at energies available at the Large Hadron Collider","total_tables":5,"type":["article"],"uuid":"cb28d6c7-6a58-4f57-832c-e01adb639d37","version":1,"year":"2023"},{"abstract":"We report about the properties of the underlying event measured with ALICE at the LHC in pp and p$-$Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV. The event activity, quantified by charged-particle number and summed-$p_{\\rm T}$ densities, is measured as a function of the leading-particle transverse momentum ($p_{\\rm T}^{\\rm trig}$). These quantities are studied in three azimuthal-angle regions relative to the leading particle in the event: toward, away, and transverse. Results are presented for three different $p_{\\rm T}$ thresholds (0.15, 0.5, and 1 GeV/$c$) at mid-pseudorapidity ($|\\eta|<0.8$). The event activity in the transverse region, which is the most sensitive to the underlying event, exhibits similar behaviour in both pp and p$-$Pb collisions, namely, a steep increase with $p_{\\rm T}^{\\rm trig}$ for low $p_{\\rm T}^{\\rm trig}$, followed by a saturation at $p_{\\rm T}^{\\rm trig} \\approx 5$ GeV/$c$. The results from pp collisions are compared with existing measurements at other centre-of-mass energies. The quantities in the toward and away regions are also analyzed after the subtraction of the contribution measured in the transverse region. The remaining jet-like particle densities are consistent in pp and p$-$Pb collisions for $p_{\\rm T}^{\\rm trig}>10$ GeV/$c$, whereas for lower $p_{\\rm T}^{\\rm trig}$ values the event activity is slightly higher in p$-$Pb than in pp collisions. The measurements are compared with predictions from the PYTHIA 8 and EPOS LHC Monte Carlo event generators.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2071174/1/csv","json":"https://www.hepdata.net/download/submission/ins2071174/1/json","root":"https://www.hepdata.net/download/submission/ins2071174/1/root","yaml":"https://www.hepdata.net/download/submission/ins2071174/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2071174/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2204.10389","authors":["Acharya, S.","Adamov\u00e1, D.","Adler, A.","Aglieri Rinella, G.","Agnello, M.","Agrawal, N.","Ahammed, Z.","Ahmad, S.","Ahn, S.U.","Ahuja, I."],"collaborations":["ALICE"],"control_number":"133032","creation_date":"2022-04-21","data":[{"abstract":"Fig. 4: Number density $N_{\\rm ch}$ (left) and $\\Sigma p_{\\rm T}$ (right) distributions as a function of $p_{\\rm T}^{\\rm trig}$ in Transverse, Away, and Toward regions for $p_{\\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071174/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2071174/Table 1/json","root":"https://www.hepdata.net/download/table/ins2071174/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2071174/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2071174/Table 1/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"133481","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["D2N/DETARAP/DPHI"],"phrases":["Proton-Proton Scattering","Inclusive","Underlying Event"],"reactions":["P P --> JET X"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.133032.v1/t1","first_author":{},"id":133481,"inspire_id":"2071174","journal_info":"JHEP 06 (2023) 023","keywords":[{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"observables","synonyms":"","value":"D2N/DETARAP/DPHI"},{"name":"reactions","synonyms":"","value":"P P --> JET X"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Underlying Event"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2022-09-13T10:07:26","parent_child_join":{"name":"child_datatable","parent":"133032"},"recid":133481,"related_publication":133032,"title":"Table 1","uuid":"e0d32a9f-fdb9-46e0-bea9-af49ef22a489"},{"abstract":"Fig. 5: Number density $N_{\\rm ch}$ (left) and $\\Sigma p_{\\rm T}$ (right) distributions as a function of $p_{\\rm T}^{\\rm trig}$ in Transverse, Away, and Toward regions for $p_{\\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071174/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2071174/Table 2/json","root":"https://www.hepdata.net/download/table/ins2071174/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2071174/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2071174/Table 2/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"133482","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["D2N/DETARAP/DPHI"],"phrases":["p-Pb","Inclusive","Underlying Event"],"reactions":["P PB --> JET X"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.133032.v1/t2","first_author":{},"id":133482,"inspire_id":"2071174","journal_info":"JHEP 06 (2023) 023","keywords":[{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"observables","synonyms":"","value":"D2N/DETARAP/DPHI"},{"name":"reactions","synonyms":"","value":"P PB --> JET X"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Underlying Event"},{"name":"phrases","synonyms":"","value":"p-Pb"}],"last_updated":"2022-09-13T10:07:26","parent_child_join":{"name":"child_datatable","parent":"133032"},"recid":133482,"related_publication":133032,"title":"Table 2","uuid":"3455ef0c-f20c-47bb-96ea-c7d3a8a8f792"},{"abstract":"Fig. 6a: Number density $N_{\\rm ch}$ (left) and $\\Sigma p_{\\rm T}$ (right) distributions as a function of $p_{\\rm T}^{\\rm trig}$ in Away and Toward regions after the subtraction of Number density $N_{\\rm ch}$ and $\\Sigma p_{\\rm T}$ distributions in the transverse region for pp collisions for $p_{\\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071174/Table 3/csv","json":"https://www.hepdata.net/download/table/ins2071174/Table 3/json","root":"https://www.hepdata.net/download/table/ins2071174/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins2071174/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2071174/Table 3/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"133483","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["D2N/DETARAP/DPHI"],"phrases":["toward (away) regions - transverse region","Inclusive","pp and p-Pb","Underlying Event"],"reactions":["P PB --> JET X","P P --> JET X"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.133032.v1/t3","first_author":{},"id":133483,"inspire_id":"2071174","journal_info":"JHEP 06 (2023) 023","keywords":[{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"observables","synonyms":"","value":"D2N/DETARAP/DPHI"},{"name":"reactions","synonyms":"","value":"P P --> JET X"},{"name":"reactions","synonyms":"","value":"P PB --> JET X"},{"name":"phrases","synonyms":"","value":"pp and p-Pb"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Underlying Event"},{"name":"phrases","synonyms":"","value":"toward (away) regions - transverse region"}],"last_updated":"2022-09-13T10:07:26","parent_child_join":{"name":"child_datatable","parent":"133032"},"recid":133483,"related_publication":133032,"title":"Table 3","uuid":"20ee3e2e-8663-4143-be80-04cd74882bd9"},{"abstract":"Fig. 6b: Number density $N_{\\rm ch}$ (left) and $\\Sigma p_{\\rm T}$ (right) distributions as a function of $p_{\\rm T}^{\\rm trig}$ in Away and Toward regions after the subtraction of Number density $N_{\\rm ch}$ and $\\Sigma p_{\\rm T}$ distributions in the transverse region for p-Pb collisions for $p_{\\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071174/Table 4/csv","json":"https://www.hepdata.net/download/table/ins2071174/Table 4/json","root":"https://www.hepdata.net/download/table/ins2071174/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins2071174/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2071174/Table 4/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"133484","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["D2N/DETARAP/DPHI"],"phrases":["toward (away) regions - transverse region","Inclusive","pp and p-Pb","Underlying Event"],"reactions":["P PB --> JET X","P P --> JET X"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.133032.v1/t4","first_author":{},"id":133484,"inspire_id":"2071174","journal_info":"JHEP 06 (2023) 023","keywords":[{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"observables","synonyms":"","value":"D2N/DETARAP/DPHI"},{"name":"reactions","synonyms":"","value":"P P --> JET X"},{"name":"reactions","synonyms":"","value":"P PB --> JET X"},{"name":"phrases","synonyms":"","value":"pp and p-Pb"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Underlying Event"},{"name":"phrases","synonyms":"","value":"toward (away) regions - transverse region"}],"last_updated":"2022-09-13T10:07:26","parent_child_join":{"name":"child_datatable","parent":"133032"},"recid":133484,"related_publication":133032,"title":"Table 4","uuid":"410d34b8-fa77-4969-acf4-49f1bb8d457e"},{"abstract":"Fig. 7a: $$ as a function of $p_{\\rm T}^{\\rm trig}$ in Toward (left) and Away (right) regions after the subtraction of transverse region for pp collisions for $p_{\\rm T} >$ 0.5 GeV/$c$. The shaded areas and the error bars around the data points represent the systematic and statistical uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2071174/Table 5/csv","json":"https://www.hepdata.net/download/table/ins2071174/Table 5/json","root":"https://www.hepdata.net/download/table/ins2071174/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins2071174/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins2071174/Table 5/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"133485","creation_date":"2022-04-21","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["PT"],"phrases":["toward (away) regions - transverse region","Inclusive","Underlying Event","pp"],"reactions":["P PB --> JET X","P P --> JET X"]},"date":"21 Apr 2022","doc_type":"datatable","doi":"10.17182/hepdata.133032.v1/t5","first_author":{},"id":133485,"inspire_id":"2071174","journal_info":"JHEP 06 (2023) 023","keywords":[{"name":"cmenergies","synonyms":"","value":"5020.0"},{"name":"observables","synonyms":"","value":"PT"},{"name":"reactions","synonyms":"","value":"P P --> JET X"},{"name":"reactions","synonyms":"","value":"P PB --> JET X"},{"name":"phrases","synonyms":"","value":"pp"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Underlying Event"},{"name":"phrases","synonyms":"","value":"toward (away) regions - transverse region"}],"last_updated":"2022-09-13T10:07:26","parent_child_join":{"name":"child_datatable","parent":"133032"},"recid":133485,"related_publication":133032,"title":"Table 5","uuid":"51209998-8dd3-4039-a8f5-04a87c5fbee0"},{"abstract":"Fig. 7b: $$ as a function of $p_{\\rm T}^{\\rm trig}$ in Toward (left) and Away (right) regions after the subtraction of transverse region for p-Pb collisions for $p_{\\rm T} >$ 0.5 GeV/$c$. 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