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collisions, a global spin polarization, $P_\\mathrm{H}$, of $\\Lambda$ and $\\bar{\\Lambda}$ hyperons along the direction of the system angular momentum was discovered and measured across a broad range of collision energies and demonstrated a trend of increasing $P_\\mathrm{H}$ with decreasing $\\sqrt{s_{NN}}$. A splitting between $\\Lambda$ and $\\bar{\\Lambda}$ polarization may be possible due to their different magnetic moments in a late-stage magnetic field sustained by the quark-gluon plasma which is formed in the collision. The results presented in this study find no significant splitting at the collision energies of $\\sqrt{s_{NN}}=19.6$ and $27$ GeV in the RHIC Beam Energy Scan Phase II using the STAR detector, with an upper limit of $P_{\\bar{\\Lambda}}-P_{\\Lambda}<0.24$% and $P_{\\bar{\\Lambda}}-P_{\\Lambda}<0.35$%, respectively, at a 95% confidence level. We derive an upper limit on the na\\\"ive extraction of the late-stage magnetic field of $B<9.4\\cdot10^{12}$ T and $B<1.4\\cdot10^{13}$ T at $\\sqrt{s_{NN}}=19.6$ and $27$ GeV, respectively, although more thorough derivations are needed. Differential measurements of $P_\\mathrm{H}$ were performed with respect to collision centrality, transverse momentum, and rapidity. With our current acceptance of $|y|<1$ and uncertainties, we observe no dependence on transverse momentum and rapidity in this analysis. These results challenge multiple existing model calculations following a variety of different assumptions which have each predicted a strong dependence on rapidity in this collision-energy range.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2659670/1/csv","json":"https://www.hepdata.net/download/submission/ins2659670/1/json","root":"https://www.hepdata.net/download/submission/ins2659670/1/root","yaml":"https://www.hepdata.net/download/submission/ins2659670/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2659670/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2305.08705","authors":["Abdulhamid, M.I.","Aboona, B.E.","Adam, J.","Adamczyk, L.","Adams, J.R.","Aggarwal, I.","Aggarwal, M.M.","Ahammed, Z.","Alpatov, E.","Anderson, D.M."],"collaborations":["STAR"],"control_number":"140936","creation_date":"2023-05-15","data":[{"abstract":"The first-order event-plane resolution determined by the STAR EPD as a function of collision centrality is roughly doubled in comparison to previous analyses using the STAR BBC. We see $R_{\\rm EP}^{(1)}$ peak for mid-central collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2659670/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2659670/Table 1/json","root":"https://www.hepdata.net/download/table/ins2659670/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2659670/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2659670/Table 1/yoda"}},"authors":null,"collaborations":["STAR"],"control_number":"144337","creation_date":"2023-05-15","data_keywords":{"cmenergies":[{"gte":27.0,"lte":27.0},{"gte":19.6,"lte":19.6}],"phrases":["Resolution"],"reactions":["Au+Au"]},"date":"15 May 2023","doc_type":"datatable","doi":"10.17182/hepdata.140936.v1/t1","first_author":{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},"id":144337,"inspire_id":"2659670","journal_info":"Phys.Rev.C 108 (2023) 014910","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au"},{"name":"cmenergies","synonyms":"","value":"19.6"},{"name":"cmenergies","synonyms":"","value":"27"},{"name":"phrases","synonyms":"","value":"Resolution"}],"last_updated":"2023-09-21T19:38:20","parent_child_join":{"name":"child_datatable","parent":"140936"},"recid":144337,"related_publication":140936,"title":"Table 1","uuid":"9d14cc59-1323-4f1f-9551-b6035b96d58f"},{"abstract":"The mid-central $P_{\\rm H}$ measurements reported in this work are shown alongside previous measurements in the upper panel, and are consistent with previous measurements at the energies studied here. The difference between integrated $P_{\\bar{\\Lambda}}$ and $P_{\\Lambda}$ is shown at $\\sqrt{s_{\\rm{NN}}}$=19.6 and 27 GeV alongside previous measurements in the lower panel. The splittings observed with these high-statistics data sets are consistent with zero. Statistical uncertainties are represented as lines while systematic uncertainties are represented as boxes. The previous $P_{\\bar{\\Lambda}}-P_{\\Lambda}$ result at $\\sqrt{s_{\\rm NN}}=7.7$ GeV is outside the axis range, but is consistent with zero within $2\\sigma$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2659670/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2659670/Table 2/json","root":"https://www.hepdata.net/download/table/ins2659670/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2659670/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2659670/Table 2/yoda"}},"authors":null,"collaborations":["STAR"],"control_number":"144338","creation_date":"2023-05-15","data_keywords":{"cmenergies":[{"gte":27.0,"lte":27.0},{"gte":19.6,"lte":19.6}],"phrases":["Polarization"],"reactions":["Au+Au"]},"date":"15 May 2023","doc_type":"datatable","doi":"10.17182/hepdata.140936.v1/t2","first_author":{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},"id":144338,"inspire_id":"2659670","journal_info":"Phys.Rev.C 108 (2023) 014910","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au"},{"name":"cmenergies","synonyms":"","value":"19.6"},{"name":"cmenergies","synonyms":"","value":"27"},{"name":"phrases","synonyms":"","value":"Polarization"}],"last_updated":"2023-09-21T19:38:20","parent_child_join":{"name":"child_datatable","parent":"140936"},"recid":144338,"related_publication":140936,"title":"Table 2","uuid":"2bb72311-f130-41f3-9f35-92b15382a08b"},{"abstract":"$P_{\\rm H}$ measurements are shown as a function of collision centrality at $\\sqrt{s_{\\rm NN}}$=19.6 and 27 GeV. Statistical uncertainties are represented as lines while systematic uncertainties are represented as boxes. $P_{\\rm H}$ increases with collision centrality at $\\sqrt{s_{\\rm NN}}$=19.6 and 27 GeV, as expected from an angular-momentum-driven phenomenon.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2659670/Table 3/csv","json":"https://www.hepdata.net/download/table/ins2659670/Table 3/json","root":"https://www.hepdata.net/download/table/ins2659670/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins2659670/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins2659670/Table 3/yoda"}},"authors":null,"collaborations":["STAR"],"control_number":"144339","creation_date":"2023-05-15","data_keywords":{"cmenergies":[{"gte":27.0,"lte":27.0},{"gte":19.6,"lte":19.6}],"phrases":["Polarization"],"reactions":["Au+Au"]},"date":"15 May 2023","doc_type":"datatable","doi":"10.17182/hepdata.140936.v1/t3","first_author":{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},"id":144339,"inspire_id":"2659670","journal_info":"Phys.Rev.C 108 (2023) 014910","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au"},{"name":"cmenergies","synonyms":"","value":"19.6"},{"name":"cmenergies","synonyms":"","value":"27"},{"name":"phrases","synonyms":"","value":"Polarization"}],"last_updated":"2023-09-21T19:38:20","parent_child_join":{"name":"child_datatable","parent":"140936"},"recid":144339,"related_publication":140936,"title":"Table 3","uuid":"d8f8b3cf-95dd-40e6-a370-9d7315726cf0"},{"abstract":"$P_{\\rm H}$ measurements are shown as a function of hyperon $p_{\\rm T}$ at $\\sqrt{s_{\\rm NN}}$=19.6 and 27 GeV. Statistical uncertainties are represented as lines while systematic uncertainties are represented as boxes. There is no observed dependence of $P_{\\rm H}$ on $p_{\\rm T}$ at $\\sqrt{s_{\\rm NN}}$=19.6 or 27 GeV, consistent with previous observations.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2659670/Table 4/csv","json":"https://www.hepdata.net/download/table/ins2659670/Table 4/json","root":"https://www.hepdata.net/download/table/ins2659670/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins2659670/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2659670/Table 4/yoda"}},"authors":null,"collaborations":["STAR"],"control_number":"144340","creation_date":"2023-05-15","data_keywords":{"cmenergies":[{"gte":27.0,"lte":27.0},{"gte":19.6,"lte":19.6}],"phrases":["Polarization"],"reactions":["Au+Au"]},"date":"15 May 2023","doc_type":"datatable","doi":"10.17182/hepdata.140936.v1/t4","first_author":{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},"id":144340,"inspire_id":"2659670","journal_info":"Phys.Rev.C 108 (2023) 014910","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au"},{"name":"cmenergies","synonyms":"","value":"19.6"},{"name":"cmenergies","synonyms":"","value":"27"},{"name":"phrases","synonyms":"","value":"Polarization"}],"last_updated":"2023-09-21T19:38:20","parent_child_join":{"name":"child_datatable","parent":"140936"},"recid":144340,"related_publication":140936,"title":"Table 4","uuid":"9392e047-808a-4392-b06d-eee9cda9c6a1"},{"abstract":"$P_{\\rm H}$ measurements are shown as a function of hyperon $y$ at $\\sqrt{s_{\\rm NN}}$=19.6 and 27 GeV. Statistical uncertainties are represented as lines while systematic uncertainties are represented as boxes. The data set at $\\sqrt{s_{\\rm NN}}$=19.6 GeV takes advantage of STAR upgrades to reach larger $|y|$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2659670/Table 5/csv","json":"https://www.hepdata.net/download/table/ins2659670/Table 5/json","root":"https://www.hepdata.net/download/table/ins2659670/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins2659670/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins2659670/Table 5/yoda"}},"authors":null,"collaborations":["STAR"],"control_number":"144341","creation_date":"2023-05-15","data_keywords":{"cmenergies":[{"gte":27.0,"lte":27.0},{"gte":19.6,"lte":19.6}],"phrases":["Polarization"],"reactions":["Au+Au"]},"date":"15 May 2023","doc_type":"datatable","doi":"10.17182/hepdata.140936.v1/t5","first_author":{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},"id":144341,"inspire_id":"2659670","journal_info":"Phys.Rev.C 108 (2023) 014910","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au"},{"name":"cmenergies","synonyms":"","value":"19.6"},{"name":"cmenergies","synonyms":"","value":"27"},{"name":"phrases","synonyms":"","value":"Polarization"}],"last_updated":"2023-09-21T19:38:20","parent_child_join":{"name":"child_datatable","parent":"140936"},"recid":144341,"related_publication":140936,"title":"Table 5","uuid":"12aa7b37-28d8-4bf0-8629-392f880a9a46"}],"data_keywords":{"cmenergies":[{"gte":27.0,"lte":27.0},{"gte":19.6,"lte":19.6}],"phrases":["Resolution","Polarization"],"reactions":["Au+Au"]},"date":"15 May 2023","doc_type":"publication","doi":"10.1103/PhysRevC.108.014910","first_author":{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},"hepdata_doi":"10.17182/hepdata.140936","id":140936,"inspire_id":"2659670","journal_info":"Phys.Rev.C 108 (2023) 014910","keywords":[{"schema":"INSPIRE","value":"beam: energy"},{"schema":"INSPIRE","value":"quark gluon: plasma"},{"schema":"INSPIRE","value":"heavy ion: scattering"},{"schema":"INSPIRE","value":"gold"},{"schema":"INSPIRE","value":"Lambda: polarization"},{"schema":"INSPIRE","value":"Antilambda: polarization"},{"schema":"INSPIRE","value":"Lambda: magnetic moment"},{"schema":"INSPIRE","value":"Antilambda: magnetic moment"},{"schema":"INSPIRE","value":"spin: polarization"},{"schema":"INSPIRE","value":"rapidity dependence"},{"schema":"INSPIRE","value":"impact parameter: dependence"},{"schema":"INSPIRE","value":"magnetic field"},{"schema":"INSPIRE","value":"splitting"},{"schema":"INSPIRE","value":"transverse momentum dependence"},{"schema":"INSPIRE","value":"hyperon"},{"schema":"INSPIRE","value":"STAR"},{"schema":"INSPIRE","value":"Brookhaven RHIC Coll"},{"schema":"INSPIRE","value":"acceptance"},{"schema":"INSPIRE","value":"Brookhaven Lab"},{"schema":"INSPIRE","value":"angular momentum"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"19.6 GeV-cms/nucleon"},{"schema":"INSPIRE","value":"27 GeV-cms/nucleon"},{"schema":"INSPIRE","value":"energy dependence"},{"schema":"INSPIRE","value":"rapidity"},{"schema":"INSPIRE","value":"transverse momentum"},{"schema":"INSPIRE","value":"hyperon: production"}],"last_updated":"2023-09-21T19:38:21","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-11T00:00:00","recid":140936,"subject_area":["nucl-ex","hep-ex"],"summary_authors":[{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},{"affiliation":"Texas A-M","full_name":"Aboona, B.E."},{"affiliation":"Prague, Tech. U.","full_name":"Adam, J."},{"affiliation":"AGH-UST, Cracow","full_name":"Adamczyk, L."},{"affiliation":"Ohio State U.","full_name":"Adams, J.R."},{"affiliation":"Panjab U., Chandigarh","full_name":"Aggarwal, I."},{"affiliation":"Panjab U., Chandigarh","full_name":"Aggarwal, M.M."},{"affiliation":"Calcutta, VECC","full_name":"Ahammed, Z."},{"affiliation":"Brookhaven","full_name":"Alpatov, E."},{"affiliation":"Texas A-M","full_name":"Anderson, D.M."}],"title":"Global polarization of $\\Lambda$ and $\\bar{\\Lambda}$ hyperons in Au+Au collisions at $\\sqrt{s_{\\rm NN}}=19.6$ and $27$ GeV","total_tables":5,"type":["article"],"uuid":"2460a0e2-8847-47e8-9737-1c8c3381cc68","version":1,"year":"2023"},{"abstract":"Global polarizations ($P$) of $\\Lambda$ ($\\bar{\\Lambda}$) hyperons have been observed in non-central heavy-ion collisions. The strong magnetic field primarily created by the spectator protons in such collisions would split the $\\Lambda$ and $\\bar{\\Lambda}$ global polarizations ($\\Delta P = P_{\\Lambda} - P_{\\bar{\\Lambda}} < 0$). Additionally, quantum chromodynamics (QCD) predicts topological charge fluctuations in vacuum, resulting in a chirality imbalance or parity violation in a local domain. This would give rise to an imbalance ($\\Delta n = \\frac{N_{\\text{L}} - N_{\\text{R}}}{\\langle N_{\\text{L}} + N_{\\text{R}} \\rangle} \\neq 0$) between left- and right-handed $\\Lambda$ ($\\bar{\\Lambda}$) as well as a charge separation along the magnetic field, referred to as the chiral magnetic effect (CME). This charge separation can be characterized by the parity-even azimuthal correlator ($\\Delta\\gamma$) and parity-odd azimuthal harmonic observable ($\\Delta a_{1}$). Measurements of $\\Delta P$, $\\Delta\\gamma$, and $\\Delta a_{1}$ have not led to definitive conclusions concerning the CME or the magnetic field, and $\\Delta n$ has not been measured previously. Correlations among these observables may reveal new insights. This paper reports measurements of correlation between $\\Delta n$ and $\\Delta a_{1}$, which is sensitive to chirality fluctuations, and correlation between $\\Delta P$ and $\\Delta\\gamma$ sensitive to magnetic field in Au+Au collisions at 27 GeV. For both measurements, no correlations have been observed beyond statistical fluctuations.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2652850/1/csv","json":"https://www.hepdata.net/download/submission/ins2652850/1/json","root":"https://www.hepdata.net/download/submission/ins2652850/1/root","yaml":"https://www.hepdata.net/download/submission/ins2652850/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2652850/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2304.10037","authors":["Abdulhamid, M.I.","Aboona, B.E.","Adam, J.","Adams, J.R.","Agakishiev, G.","Aggarwal, I.","Aggarwal, M.M.","Ahammed, Z.","Aitbaev, A.","Alekseev, I."],"collaborations":["STAR"],"control_number":"140262","creation_date":"2023-04-19","data":[{"abstract":"Figure 1","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2652850/Figure 1/csv","json":"https://www.hepdata.net/download/table/ins2652850/Figure 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Non-central collisions can produce strong magnetic fields on the order of $10^{18}$ Gauss, which offers a probe into the electrical conductivity of the QGP. In particular, quarks and anti-quarks carry opposite charges and receive contrary electromagnetic forces that alter their momenta. This phenomenon can be manifested in the collective motion of final-state particles, specifically in the rapidity-odd directed flow, denoted as $v_1(\\mathsf{y})$. Here we present the charge-dependent measurements of $dv_1/d\\mathsf{y}$ near midrapidities for $\\pi^{\\pm}$, $K^{\\pm}$, and $p(\\bar{p})$ in Au+Au and isobar ($_{44}^{96}$Ru+$_{44}^{96}$Ru and $_{40}^{96}$Zr+$_{40}^{96}$Zr) collisions at $\\sqrt{s_{\\rm NN}}=$ 200 GeV, and in Au+Au collisions at 27 GeV, recorded by the STAR detector at the Relativistic Heavy Ion Collider. The combined dependence of the $v_1$ signal on collision system, particle species, and collision centrality can be qualitatively and semi-quantitatively understood as several effects on constituent quarks. While the results in central events can be explained by the $u$ and $d$ quarks transported from initial-state nuclei, those in peripheral events reveal the impacts of the electromagnetic field on the QGP. 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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. For the reference branching ratio, the most stringent limits are used.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Table 7/csv","json":"https://www.hepdata.net/download/table/ins2627201/Table 7/json","root":"https://www.hepdata.net/download/table/ins2627201/Table 7/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Table 7/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Table 7/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145906","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145906,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145906,"related_publication":145074,"title":"Table 7","uuid":"65e1f00a-7a13-4f3c-a3ff-6293b5107984"},{"abstract":"Observed and expected 95% CL limits on the FCNC $t\\rightarrow Zq$ branching ratios and the effective coupling strengths for different vertices and couplings (top eight rows). For the latter, the energy scale is assumed to be $\\Lambda_{NP}$ = 1 TeV. The bottom rows show, for the case of the FCNC $t\\rightarrow Zu$ branching ratio, the observed and expected 95% CL limits when only one of the two SRs, either SR1 or SR2, and all CRs are included in the likelihood.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Table 8/csv","json":"https://www.hepdata.net/download/table/ins2627201/Table 8/json","root":"https://www.hepdata.net/download/table/ins2627201/Table 8/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Table 8/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Table 8/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145907","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145907,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145907,"related_publication":145074,"title":"Table 8","uuid":"edd0b7d3-0c80-45ff-830a-14a38b8fa2e5"},{"abstract":"Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the SM top-quark candidate in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 02a/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145908","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DM"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145908,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DM"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145908,"related_publication":145074,"title":"Figure 02a","uuid":"79a808ba-6d17-4bf5-bf2d-5d8db6457418"},{"abstract":"Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the FCNC top-quark candidate in SR1. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). The lower panels show the ratios of the data (Data) to the background prediction (Bkg.).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/csv","json":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/json","root":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/root","yaml":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/yaml","yoda":"https://www.hepdata.net/download/table/ins2627201/Figure 02b/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"145909","creation_date":"2023-01-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["DN/DM"],"phrases":["Neutral Current","Top"],"reactions":["P P --> TQ TQBAR --> Z0 UQ W- BQBAR","P P --> TQ TQBAR --> Z0 CQ W- BQBAR","P P --> TQ Z0"]},"date":"27 Jan 2023","doc_type":"datatable","doi":"10.17182/hepdata.145074.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, G."},"id":145909,"inspire_id":"2627201","journal_info":"Phys.Rev.D 108 (2023) 032019","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"observables","synonyms":"","value":"DN/DM"},{"name":"phrases","synonyms":"","value":"Top"},{"name":"phrases","synonyms":"","value":"Neutral Current"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 UQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ TQBAR --> Z0 CQ W- BQBAR"},{"name":"reactions","synonyms":"","value":"P P --> TQ Z0"}],"last_updated":"2023-12-15T10:09:14","parent_child_join":{"name":"child_datatable","parent":"145074"},"recid":145909,"related_publication":145074,"title":"Figure 02b","uuid":"7106f9ca-6799-4511-854e-61672aad6367"},{"abstract":"Comparison between data and background prediction before the fit (Pre-Fit) for the mass of the SM top-quark candidate in SR2. The uncertainty band includes both the statistical and systematic uncertainties in the background prediction. The four FCNC LH signals are also shown separately, normalized to five times the cross-section corresponding to the most stringent observed branching ratio limits. The first (last) bin in all distributions includes the underflow (overflow). 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The 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={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. 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While the $v_2(p_{\\mathrm{T}})$ values depend on the colliding systems, the $v_3(p_{\\mathrm{T}})$ values are system-independent within the uncertainties, suggesting an influence on eccentricity from sub-nucleonic fluctuations in these small-sized systems. These results also provide stringent constraints for the hydrodynamic modeling of these systems.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2167879/1/csv","json":"https://www.hepdata.net/download/submission/ins2167879/1/json","root":"https://www.hepdata.net/download/submission/ins2167879/1/root","yaml":"https://www.hepdata.net/download/submission/ins2167879/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2167879/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2210.11352","authors":["Abdulhamid, M.I.","Aboona, B.E.","Adam, J.","Adams, J.R.","Agakishiev, G.","Aggarwal, I.","Aggarwal, M.M.","Ahammed, Z.","Aitbaev, A.","Alekseev, I."],"collaborations":["STAR"],"control_number":"134955","creation_date":"2022-10-20","data":[{"abstract":"v2 and v3 in 0-10% He+Au collisions at 200 GeV","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2167879/Figure 3_a_b/csv","json":"https://www.hepdata.net/download/table/ins2167879/Figure 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"}],"last_updated":"2023-06-30T02:30:53","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-12-11T00:00:00","recid":134955,"subject_area":["nucl-ex"],"summary_authors":[{"affiliation":"American U., Cairo","full_name":"Abdulhamid, M.I."},{"affiliation":"Texas A-M","full_name":"Aboona, B.E."},{"affiliation":"Prague, Tech. U.","full_name":"Adam, J."},{"affiliation":"Ohio State U.","full_name":"Adams, J.R."},{"affiliation":"Dubna, JINR","full_name":"Agakishiev, G."},{"affiliation":"Panjab U., Chandigarh","full_name":"Aggarwal, I."},{"affiliation":"Panjab U., Chandigarh","full_name":"Aggarwal, M.M."},{"affiliation":"Calcutta, VECC","full_name":"Ahammed, Z."},{"affiliation":"Dubna, JINR","full_name":"Aitbaev, A."},{"affiliation":"Moscow, ITEP","full_name":"Alekseev, I."}],"title":"Measurements of the elliptic and triangular azimuthal anisotropies in central $^{3}$He+Au, $d$+Au and $p$+Au collisions at $\\mbox{$\\sqrt{s_{\\mathrm{NN}}}$}$ = 200 GeV","total_tables":5,"type":["article"],"uuid":"37e0ade2-febc-42fd-8f01-df76d2e77eb2","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. 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