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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. 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We measure five angular-asymmetry observables as functions of the decay recoil that are sensitive to lepton-universality-violating contributions. We use events where one neutral $B$ is fully reconstructed in $\\Upsilon\\left(4S\\right)\\to{}B \\overline{B}$ decays in data corresponding to $189~\\mathrm{fb}^{-1}$ integrated luminosity from electron-positron collisions collected with the Belle II detector. We find no significant deviation from the standard model expectations.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2685572/1/csv","json":"https://www.hepdata.net/download/submission/ins2685572/1/json","root":"https://www.hepdata.net/download/submission/ins2685572/1/root","yaml":"https://www.hepdata.net/download/submission/ins2685572/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2685572/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2308.02023","authors":["Adachi, I.","Adamczyk, K.","Aggarwal, L.","Aihara, H.","Akopov, N.","Aloisio, A.","Anh Ky, N.","Asner, D.M.","Atmacan, H.","Aushev, T."],"collaborations":["Belle-II"],"control_number":"144759","creation_date":"2023-08-03","data":[{"abstract":"Observed values of all angular asymmetry variables.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2685572/Central values/csv","json":"https://www.hepdata.net/download/table/ins2685572/Central 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The asymmetries are consistent with zero, similar to those for midrapidity neutral pions and eta mesons produced in $p$+$p$ collisions. These measurements show no evidence of additional effects that could potentially arise from the more complex partonic environment present in proton-nucleus collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2641468/1/csv","json":"https://www.hepdata.net/download/submission/ins2641468/1/json","root":"https://www.hepdata.net/download/submission/ins2641468/1/root","yaml":"https://www.hepdata.net/download/submission/ins2641468/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2641468/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2303.07190","authors":["Abdulameer, N.J.","Acharya, U.","Aidala, C.","Akiba, Y.","Alfred, M.","Andrieux, V.","Apadula, N.","Asano, H.","Azmoun, B.","Babintsev, V."],"collaborations":["PHENIX"],"control_number":"139098","creation_date":"2023-03-13","data":[{"abstract":"Data from Figure 2 (a) of the $\\pi^{0}$ transverse single-spin asymmetry in $\\sqrt{s_{NN}}=200$ GeV $p^{\\uparrow}+$Au and $p^{\\uparrow}+$Al 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$\\pi^{0}$ and $\\eta$ mesons in $p$+Au and $p$+Al collisions at $\\sqrt{s_{_{NN}}}=$ 200 GeV","total_tables":2,"type":["article"],"uuid":"7099a3d6-7cfd-4c03-b8a0-969940b46c7b","version":1,"year":"2023"},{"abstract":"A precision measurement of the matrix elements for $\\eta\\to\\pi^+\\pi^-\\pi^0$ and $\\eta\\to\\pi^0\\pi^0\\pi^0$ decays is performed using a sample of $(10087\\pm44)\\times10^6$$J/\\psi$ decays collected with the BESIII detector. The decay $J/\\psi \\to \\gamma \\eta$ is used to select clean samples of 631,686 $\\eta\\to\\pi^+\\pi^-\\pi^0$ decays and 272,322 $\\eta\\to\\pi^0\\pi^0\\pi^0$ decays. The matrix elements for both channels are in reasonable agreement with previous measurements. The non-zero $gX^2Y$ term for the decay mode $\\eta\\to\\pi^+\\pi^-\\pi^0$ is confirmed, as reported by the KLOE Collaboration, while the other higher-order terms are found to be insignificant. Dalitz plot asymmetries in the $\\eta\\to\\pi^+\\pi^-\\pi^0$ decay are also explored and are found to be consistent with charge conjugation invariance. In addition, a cusp effect is investigated in the $\\eta\\to\\pi^0\\pi^0\\pi^0$ decay, and no obvious structure around the $\\pi^+\\pi^-$ mass threshold is observed.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2633025/1/csv","json":"https://www.hepdata.net/download/submission/ins2633025/1/json","root":"https://www.hepdata.net/download/submission/ins2633025/1/root","yaml":"https://www.hepdata.net/download/submission/ins2633025/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2633025/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2302.08282","authors":["Ablikim, M.","Achasov, M.N.","Adlarson, P.","Aliberti, R.","Amoroso, A.","An, M.R.","An, Q.","Bai, Y.","Bakina, O.","Balossino, I."],"collaborations":["BESIII"],"control_number":"141285","creation_date":"2023-02-16","data":[{"abstract":"The acceptance corrected $\\eta\\to\\pi^+\\pi^-\\pi^0$ data from 10 billion $J/\\psi$ events collected at BESIII and the corresponding statistical uncertainties in the Dalitz plot variables $X$ and $Y$. 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This so-called Gaussian Estimator allows for the first time the study of these quantities without the influence of correlations between different flow amplitudes. The centrality dependence of various correlations between two, three and four symmetry planes is presented. The ordering of magnitude between these symmetry plane correlations is discussed and the results of the Gaussian Estimator are compared with measurements of previously used estimators. The results utilizing the new estimator lead to significantly smaller correlations than reported by studies using the Scalar Product method. Furthermore, the obtained symmetry plane correlations are compared to state-of-the-art hydrodynamic model calculations for the evolution of heavy-ion collisions. While the model predictions provide a qualitative description of the data, quantitative agreement is not always observed, particularly for correlators with significant non-linear response of the medium to initial state anisotropies of the collision system. 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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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matter"},{"schema":"INSPIRE","value":"correlation"},{"schema":"INSPIRE","value":"estimator"},{"schema":"INSPIRE","value":"TeV"},{"schema":"INSPIRE","value":"nonlinear"},{"schema":"INSPIRE","value":"correlation function"},{"schema":"INSPIRE","value":"flow"},{"schema":"INSPIRE","value":"ALICE"},{"schema":"INSPIRE","value":"Bayesian"}],"last_updated":"2023-06-02T13:53:08","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-02-28T00:00:00","recid":141027,"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":"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. 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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 uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 02d/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145911","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DPT"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145911,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DPT"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145911,"related_publication":145074,"title":"Figure 02d","uuid":"f8f1e742-4253-4495-b8ea-112df51ad4a7"},{"abstract":"Comparison between data and background prediction after the fit to data (Post-Fit) for the FCNC tZu LH coupling extraction. The distribution is for the $D_{1}$ discriminant in the mass sideband CR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The FCNC tZu LH signals are also separately shown, normalized to 500 times the best fit of the signal yield. 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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. 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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. 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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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The bounds are derived from the $A_C^{t\\bar{t}}$ inclusive measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. 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Measurements were performed via the $\\phi\\rightarrow K^{+}K^{-}$ decay channel at midrapidity $|\\eta|<0.35$. Features of $\\phi$-meson production measured in Cu$+$Cu, Cu$+$Au, Au$+$Au, and U$+$U collisions were found to not depend on the collision geometry, which was expected because the yields are averaged over the azimuthal angle and follow the expected scaling with nuclear-overlap size. The elliptic flow of the $\\phi$ meson in Cu$+$Au, Au$+$Au, and U$+$U collisions scales with second-order-participant eccentricity and the length scale of the nuclear-overlap region (estimated with the number of participating nucleons). At moderate $p_T$, $\\phi$-meson production measured in Cu$+$Au and U$+$U collisions is consistent with coalescence-model predictions, whereas at high $p_T$ the production is in agreement with expectations for in-medium energy loss of parent partons prior to their fragmentation. The elliptic flow for $\\phi$ mesons measured in Cu$+$Au and U$+$U collisions is well described by a (2+1)D viscous-hydrodynamic model with specific-shear viscosity $\\eta/s=1/4\\pi$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2623245/1/csv","json":"https://www.hepdata.net/download/submission/ins2623245/1/json","root":"https://www.hepdata.net/download/submission/ins2623245/1/root","yaml":"https://www.hepdata.net/download/submission/ins2623245/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2623245/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2207.10745","authors":["Abdulameer, N.J.","Acharya, U.","Aidala, C.","Ajitanand, N.N.","Akiba, Y.","Akimoto, R.","Alexander, J.","Alfred, M.","Finger, M., Jr.","Finger, M."],"collaborations":["PHENIX"],"control_number":"132483","creation_date":"2022-07-21","data":[{"abstract":"Invariant transverse momentum spectra measured for $\\phi$ mesons in (a) Cu+Au and (b) U+U collisions at $\\sqrt{s}$ = 200 GeV at midrapidity","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2623245/Figure3ab/csv","json":"https://www.hepdata.net/download/table/ins2623245/Figure3ab/json","root":"https://www.hepdata.net/download/table/ins2623245/Figure3ab/root","yaml":"https://www.hepdata.net/download/table/ins2623245/Figure3ab/yaml","yoda":"https://www.hepdata.net/download/table/ins2623245/Figure3ab/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"133536","creation_date":"2022-07-21","data_keywords":{"cmenergies":[{"gte":193.0,"lte":193.0},{"gte":200.0,"lte":200.0}],"phrases":["Invariant transverse momentum spectra","ppg242","$\\phi$"],"reactions":["U U --> NEUTRAL X","CU AU --> NEUTRAL X"]},"date":"21 Jul 2022","doc_type":"datatable","doi":"10.17182/hepdata.132483.v1/t1","first_author":{"affiliation":"Debrecen U.","full_name":"Abdulameer, N.J."},"id":133536,"inspire_id":2623245,"journal_info":"Phys.Rev.C 107 (2023) 014907","keywords":[{"name":"reactions","synonyms":"","value":"U U --> NEUTRAL X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"cmenergies","synonyms":"","value":"193.0"},{"name":"phrases","synonyms":"","value":"ppg242"},{"name":"phrases","synonyms":"","value":"$\\phi$"},{"name":"phrases","synonyms":"","value":"Invariant transverse momentum spectra"},{"name":"reactions","synonyms":"","value":"CU AU --> NEUTRAL X"}],"last_updated":"2023-04-10T20:49:29","parent_child_join":{"name":"child_datatable","parent":"132483"},"recid":133536,"related_publication":132483,"title":"Figure3ab","uuid":"a341771a-3022-4c06-8812-6bef41248a58"},{"abstract":"Invariant transverse momentum spectra measured for $\\phi$ mesons in (c) Cu+Au and (d) U+U collisions at $\\sqrt{s}$ = 200 GeV at midrapidity. 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The normalization uncertainty from p+p of about $\\sim9.7\\%$ is not shown.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2623245/Figure4/csv","json":"https://www.hepdata.net/download/table/ins2623245/Figure4/json","root":"https://www.hepdata.net/download/table/ins2623245/Figure4/root","yaml":"https://www.hepdata.net/download/table/ins2623245/Figure4/yaml","yoda":"https://www.hepdata.net/download/table/ins2623245/Figure4/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"133538","creation_date":"2022-07-21","data_keywords":{"cmenergies":[{"gte":193.0,"lte":193.0},{"gte":200.0,"lte":200.0}],"phrases":["nuclear modification factors","ppg242","$\\phi$"],"reactions":["U U --> NEUTRAL X","CU AU --> NEUTRAL X"]},"date":"21 Jul 2022","doc_type":"datatable","doi":"10.17182/hepdata.132483.v1/t3","first_author":{"affiliation":"Debrecen U.","full_name":"Abdulameer, N.J."},"id":133538,"inspire_id":2623245,"journal_info":"Phys.Rev.C 107 (2023) 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