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This analysis supersedes and expands upon the previous nonresonant ATLAS results in this final state based on the same data sample. The analysis strategy is optimised to probe anomalous values not only of the Higgs ($H$) boson self-coupling modifier $\\kappa_\\lambda$ but also of the quartic $HHVV$ ($V=W,Z$) coupling modifier $\\kappa_{2V}$. No significant excess above the expected background from Standard Model processes is observed. An observed upper limit $\\mu_{HH}<4.0$ is set at 95% confidence level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The 95% confidence intervals for the coupling modifiers are $-1.4<\\kappa_\\lambda<6.9$ and $-0.5<\\kappa_{2V}<2.7$, assuming all other Higgs boson couplings except the one under study are fixed to the Standard Model predictions. 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The multiparticle cumulant technique is used to obtain the elliptic flow coefficients $v_2\\{2\\}$, $v_2\\{4\\}$, $v_2\\{6\\}$, and $v_2\\{8\\}$, and triangular flow coefficients $v_3\\{2\\}$ and $v_3\\{4\\}$. Using the small-variance limit, we estimate the mean and variance of the event-by-event $v_2$ distribution from $v_2\\{2\\}$ and $v_2\\{4\\}$. In a complementary analysis, we also use a folding procedure to study the distributions of $v_2$ and $v_3$ directly, extracting both the mean and variance. 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(b) The black points indicate $v_2${4} with no pseudorapidity gap, the blue points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 but where some short-range pairs are allowed, and the red points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 where no short-range pairs are allowed.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.1/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.1/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.1/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.1/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.1/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150509","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t1","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150509,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150509,"related_publication":150019,"title":"Figure 6a pt.1","uuid":"59fc16d7-39e4-4ec6-b1ae-15ce5fc15b72"},{"abstract":"Centrality dependence of (a) $v_2${2} and (b) $v_2${4}. 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(b) The black points indicate $v_2${4} with no pseudorapidity gap, the blue points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 but where some short-range pairs are allowed, and the red points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 where no short-range pairs are allowed.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.2/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.2/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.2/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.2/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 6a pt.2/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150510","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t2","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150510,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150510,"related_publication":150019,"title":"Figure 6a pt.2","uuid":"04272ea9-153c-4d19-b8e8-80cb64e7c206"},{"abstract":"Centrality dependence of (a) $v_2${2} and (b) $v_2${4}. 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(b) The black points indicate $v_2${4} with no pseudorapidity gap, the blue points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 but where some short-range pairs are allowed, and the red points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 where no short-range pairs are allowed.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.1/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.1/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.1/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.1/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.1/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150511","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t3","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150511,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150511,"related_publication":150019,"title":"Figure 6b pt.1","uuid":"d3ba7dbf-2308-4865-9bd2-86ca81b5f2ef"},{"abstract":"Centrality dependence of (a) $v_2${2} and (b) $v_2${4}. 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(b) The black points indicate $v_2${4} with no pseudorapidity gap, the blue points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 but where some short-range pairs are allowed, and the red points indicate a two-subevent method with |$\\Delta\\eta$| > 2.0 where no short-range pairs are allowed.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.2/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.2/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.2/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.2/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 6b pt.2/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150512","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t4","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150512,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150512,"related_publication":150019,"title":"Figure 6b pt.2","uuid":"d1f270f7-ee60-4d05-98c4-698d6dc53d9b"},{"abstract":"Centrality dependence of (a) $v_2${2} and (b) $v_2${4}. 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The magenta open diamonds indicate the $v_2${SP }, the blue open squares indicate $v_2${4}, the black open circles indicate $v_2${6}, and the green filled diamonds indicate $v_2${8}.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 7d/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 7d/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 7d/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 7d/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 7d/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150517","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t9","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150517,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150517,"related_publication":150019,"title":"Figure 7d","uuid":"8d3ac072-af06-4f7c-b591-cbe1b02c252b"},{"abstract":"Cumulant method estimate of $\\sigma_{v_{2}}$ / $\\langle v_{2} \\rangle$ as a function of centrality in Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV. The data are shown as black open squares. The same calculation as done in data is done in ampt, shown as a solid green line. Calculations of $\\sigma_{\\epsilon_{2}}$ /$ \\langle\\epsilon_{2}\\rangle$ performed in the Monte Carlo Glauber model are shown as blue lines. The solid blue line is the Monte Carlo Glauber calculation done using the same estimate as the data, the dashed blue line is the direct calculation of the moments of the MC Glauber $\\epsilon_{2}$ distribution.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 8/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 8/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 8/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 8/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 8/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150518","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t10","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150518,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150518,"related_publication":150019,"title":"Figure 8","uuid":"117c96c7-17ff-478c-a3ff-23251a7b488e"},{"abstract":"Centrality dependence of $v_3${2, |$\\Delta\\eta$| > 2} in Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV, shown as magenta diamonds. The systematic uncertainty is indicated as a shaded magenta band. Also shown as black squares are $\\sqrt{\\langle v^{2}_{3}\\rangle}$ as determined from the folding analysis, which is shown in the next section.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 9a/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 9a/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 9a/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 9a/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 9a/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150519","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t11","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150519,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150519,"related_publication":150019,"title":"Figure 9a","uuid":"7a0451ee-c052-4093-8a95-2dbfc7c7c00e"},{"abstract":"Centrality dependence of $v_3${2, |$\\Delta\\eta$| > 2} in Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV, shown as magenta diamonds. The systematic uncertainty is indicated as a shaded magenta band. Also shown as black squares are $\\sqrt{\\langle v^{2}_{3}\\rangle}$ as determined from the folding analysis, which is shown in the next section.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 9b/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 9b/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 9b/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 9b/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 9b/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150520","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t12","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150520,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150520,"related_publication":150019,"title":"Figure 9b","uuid":"0631b7ae-57f6-4a26-9dbd-64baa91f2d26"},{"abstract":"Centrality dependence of $c_3${4} for Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV. (a) Calculations using both arms: $c_3${4} (black circles), $c_3${4}$_{ab|ab}$ (blue diamonds), $c_3${4}$_{aa|bb}$ (red squares), and comparison to STAR [36] (black stars). (b) Comparison of $c_3${4} determined using both arms (open symbols) and a single arm (closed symbols). Note that the open black circles are the same in (a) and (b).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.1/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.1/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.1/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.1/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.1/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150521","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t13","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150521,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150521,"related_publication":150019,"title":"Figure 10a pt.1","uuid":"33ff6ced-de0b-44e7-be77-f3a7fc09c65c"},{"abstract":"Centrality dependence of $c_3${4} for Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV. (a) Calculations using both arms: $c_3${4} (black circles), $c_3${4}$_{ab|ab}$ (blue diamonds), $c_3${4}$_{aa|bb}$ (red squares), and comparison to STAR [36] (black stars). (b) Comparison of $c_3${4} determined using both arms (open symbols) and a single arm (closed symbols). Note that the open black circles are the same in (a) and (b).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.2/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.2/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.2/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.2/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 10a pt.2/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150522","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t14","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150522,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150522,"related_publication":150019,"title":"Figure 10a pt.2","uuid":"eb1ebbbf-f4fc-4d5d-8cea-1a3f698e8c92"},{"abstract":"Centrality dependence of $c_3${4} for Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV. (a) Calculations using both arms: $c_3${4} (black circles), $c_3${4}$_{ab|ab}$ (blue diamonds), $c_3${4}$_{aa|bb}$ (red squares), and comparison to STAR [36] (black stars). (b) Comparison of $c_3${4} determined using both arms (open symbols) and a single arm (closed symbols). Note that the open black circles are the same in (a) and (b).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 10b/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 10b/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 10b/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 10b/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 10b/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150523","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t15","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150523,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150523,"related_publication":150019,"title":"Figure 10b","uuid":"ca8706d1-a6fe-4271-bf68-f7753c78e3d6"},{"abstract":"Folding results for (a) $v_2$, (b) $\\sigma_{v_{2}}$ , and (c) $\\sigma_{v_{2}}$ / $\\langle v_{2}\\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. In the case of $\\langle v_{2}\\rangle$, the statistical uncertainties at the 68.27% confidence level are too small to be seen, and the uncertainties at the 95.45% confidence level are visible but noticeably smaller than the marker size. Shown as blue squares are the same quantities as determined using the cumulant based calculation\u2014these points are slightly offset in the x-coordinate to improve visibility.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 11a/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 11a/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 11a/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 11a/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 11a/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150524","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t16","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150524,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150524,"related_publication":150019,"title":"Figure 11a","uuid":"8c100ced-3160-4a01-9944-d621990f49e4"},{"abstract":"Folding results for (a) $v_2$, (b) $\\sigma_{v_{2}}$ , and (c) $\\sigma_{v_{2}}$ / $\\langle v_{2}\\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. In the case of $\\langle v_{2}\\rangle$, the statistical uncertainties at the 68.27% confidence level are too small to be seen, and the uncertainties at the 95.45% confidence level are visible but noticeably smaller than the marker size. Shown as blue squares are the same quantities as determined using the cumulant based calculation\u2014these points are slightly offset in the x-coordinate to improve visibility.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 11b/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 11b/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 11b/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 11b/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 11b/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150525","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t17","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150525,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150525,"related_publication":150019,"title":"Figure 11b","uuid":"75ec6929-d7dc-4d7e-bce8-53005c3656ff"},{"abstract":"Folding results for (a) $v_2$, (b) $\\sigma_{v_{2}}$ , and (c) $\\sigma_{v_{2}}$ / $\\langle v_{2}\\rangle$. 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The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. 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The $\\sigma_{v_{3}}$ /$\\langle v_{3}\\rangle$ values are all \u2248 0.52, the apparent limiting value of this quantity for the Bessel-Gaussian distribution.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 12b/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 12b/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 12b/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 12b/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 12b/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150528","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t20","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150528,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150528,"related_publication":150019,"title":"Figure 12b","uuid":"443d3c1a-ed0d-4734-9525-f346a8c13768"},{"abstract":"Folding results for (a) $\\langle v_{3}\\rangle$, (b) $\\sigma_{v_{3}}$ , and (c) $\\sigma_{v_{3}}$ /$\\langle v_{3}\\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. The $\\sigma_{v_{3}}$ /$\\langle v_{3}\\rangle$ values are all \u2248 0.52, the apparent limiting value of this quantity for the Bessel-Gaussian distribution.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1670164/Figure 12c/csv","json":"https://www.hepdata.net/download/table/ins1670164/Figure 12c/json","root":"https://www.hepdata.net/download/table/ins1670164/Figure 12c/root","yaml":"https://www.hepdata.net/download/table/ins1670164/Figure 12c/yaml","yoda":"https://www.hepdata.net/download/table/ins1670164/Figure 12c/yoda"}},"authors":null,"collaborations":["PHENIX"],"control_number":"150529","creation_date":"2018-04-26","data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"datatable","doi":"10.17182/hepdata.150019.v1/t21","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"id":150529,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"name":"reactions","synonyms":"","value":"Au+Au$\\implies$ CHARGED X"},{"name":"cmenergies","synonyms":"","value":"200.0"},{"name":"phrases","synonyms":"","value":"ppg218"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"elliptic flow"},{"name":"phrases","synonyms":"","value":"triangular flow"}],"last_updated":"2024-03-25T14:45:42","parent_child_join":{"name":"child_datatable","parent":"150019"},"recid":150529,"related_publication":150019,"title":"Figure 12c","uuid":"581a4add-f759-4122-9cc8-49d7f9ab3ded"}],"data_keywords":{"cmenergies":[{"gte":200.0,"lte":200.0}],"phrases":["triangular flow","ppg218","elliptic flow","azimuthal anisotropy"],"reactions":["Au+Au$\\implies$ CHARGED X"]},"date":"26 Apr 2018","doc_type":"publication","doi":"10.1103/PhysRevC.99.024903","first_author":{"affiliation":"Colorado U.","full_name":"Adare, A."},"hepdata_doi":"10.17182/hepdata.150019","id":150019,"inspire_id":"1670164","journal_info":"Phys.Rev.C 99 (2019) 024903","keywords":[{"source":"publisher","value":"Relativistic Nuclear Collisions"},{"schema":"INSPIRE","value":"fluctuation: geometrical"},{"schema":"INSPIRE","value":"angular distribution: anisotropy"},{"schema":"INSPIRE","value":"heavy ion: scattering"},{"schema":"INSPIRE","value":"elliptic flow"},{"schema":"INSPIRE","value":"triangular flow"},{"schema":"INSPIRE","value":"angular correlation"},{"schema":"INSPIRE","value":"momentum spectrum"},{"schema":"INSPIRE","value":"charged particle"},{"schema":"INSPIRE","value":"rapidity"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"200 GeV-cms/nucleon"}],"last_updated":"2024-03-25T14:45:45","parent_child_join":{"name":"parent_publication"},"publication_date":"2019-03-27T00:00:00","recid":150019,"subject_area":["hep-ex","nucl-ex"],"summary_authors":[{"affiliation":"Colorado U.","full_name":"Adare, A."},{"affiliation":"Michigan U.","full_name":"Aidala, C."},{"affiliation":"Nishina Ctr., RIKEN","full_name":"Ajitanand, N.N."},{"affiliation":"Nishina Ctr., RIKEN","full_name":"Akiba, Y."},{"affiliation":"Howard U.","full_name":"Alfred, M."},{"affiliation":"Iowa State U.","full_name":"Apadula, N."},{"affiliation":"Kyoto U.","full_name":"Asano, H."},{"affiliation":"Brookhaven","full_name":"Azmoun, B."},{"affiliation":"Serpukhov, IHEP","full_name":"Babintsev, V."},{"affiliation":"Eotvos U.","full_name":"Bagoly, A."}],"title":"Multi-particle azimuthal correlations for extracting event-by-event elliptic and triangular flow in Au$+$Au collisions at $\\sqrt{s_{_{NN}}}=200$ GeV","total_tables":21,"type":["article"],"uuid":"ca26d97e-e6da-42d7-90ca-a9522952b5d8","version":1,"year":"2019"},{"abstract":"Charged-particle jet yields have been measured in semicentral Pb$-$Pb collisions at center-of-mass energy per nucleon-nucleon collision $\\sqrt{s_{\\rm NN}} = 5$ TeV with the ALICE detector at the LHC. These yields are reported as a function of the jet transverse momentum, and further classified by their angle with respect to the event plane and the event shape, characterized by ellipticity, in an effort to study the path-length dependence of jet quenching. Jets were reconstructed at midrapidity from charged-particle tracks using the anti-$k_{\\rm T}$ algorithm with resolution parameters $R =$ 0.2 and 0.4, with event-plane angle and event-shape values determined using information from forward scintillating detectors. The results presented in this letter show that, in semicentral Pb$-$Pb collisions, there is no significant difference between jet yields in predominantly isotropic and elliptical events. However, out-of-plane jets are observed to be more suppressed than in-plane jets. Further, this relative suppression is greater for low transverse momentum ($<$ 50 GeV/$c$) $R =$ 0.2 jets produced in elliptical events, with out-of-plane to in-plane jet-yield ratios varying up to 5.2$\\sigma$ between different event-shape classes. These results agree with previous studies indicating that jets experience azimuthally anisotropic suppression when traversing the QGP medium, and can provide additional constraints on the path-length dependence of jet energy loss.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2681682/1/csv","json":"https://www.hepdata.net/download/submission/ins2681682/1/json","root":"https://www.hepdata.net/download/submission/ins2681682/1/root","yaml":"https://www.hepdata.net/download/submission/ins2681682/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2681682/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2307.14097","authors":["Acharya, Shreyasi","Adamova, Dagmar","Aglieri Rinella, Gianluca","Agnello, Michelangelo","Agrawal, Neelima","Ahammed, Zubayer","Ahmad, Shakeel","Ahn, Sang Un","Ahuja, Ishaan","Akindinov, Alexander"],"collaborations":["ALICE"],"control_number":"150418","creation_date":"2023-07-26","data":[{"abstract":"Charged-particle jet yields, 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The analysis is performed using a data sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb$^{-1}$. To reduce the background from standard model processes, the search requires the Higgs boson to be produced in association with a leptonically decaying W or Z boson. The analysis probes the production of new light bosons in a 15 $\\lt$$m_\\mathrm{a}$$\\lt$ 60 GeV mass range. Assuming the standard model predictions for the Higgs boson production cross sections for pp $\\to$ WH and ZH, model independent upper limits at 95% confidence level are derived for the branching fraction $\\mathcal{B}$(H $\\to$ aa $\\to$ $\\mathrm{b\\bar{b}b\\bar{b}}$). The combined WH and ZH observed upper limit on the branching fraction ranges from 1.10 for $m_\\mathrm{a} =$ 20 GeV to 0.36 for $m_\\mathrm{a} =$ 60 GeV, complementing other measurements in the $\\mu\\mu\\tau\\tau$, $\\tau\\tau\\tau\\tau$ and bb$\\ell\\ell$ ($\\ell=$ $\\mu$,$\\tau$) channels.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2769284/1/csv","json":"https://www.hepdata.net/download/submission/ins2769284/1/json","root":"https://www.hepdata.net/download/submission/ins2769284/1/root","yaml":"https://www.hepdata.net/download/submission/ins2769284/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2769284/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2403.10341","authors":["Hayrapetyan, Aram","Tumasyan, Armen","Adam, Wolfgang","Andrejkovic, Janik Walter","Bergauer, Thomas","Chatterjee, Suman","Damanakis, Konstantinos","Dragicevic, Marko","Hussain, Priya Sajid","Jeitler, Manfred"],"collaborations":["CMS"],"control_number":"147309","creation_date":"2024-03-15","data":[{"abstract":"Post-fit BDT distributions in the WH channel extracted with the ma = 60 GeV signal hypothesis. Signal regions for the 3b (upper) and 4b (lower) event categories are shown separately for the electron (left) and muon (right) channels. The dotted lines WH20 GeV, WH60 GeV, illustrate the shapes of the signal template normalised to the SM cross section times a branching fraction B(H \u2192 aa \u2192 bbbb) = 1 and scaled by the factors indicated in the figure. The horizontal error bars indicate the bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2769284/Figure 1/csv","json":"https://www.hepdata.net/download/table/ins2769284/Figure 1/json","root":"https://www.hepdata.net/download/table/ins2769284/Figure 1/root","yaml":"https://www.hepdata.net/download/table/ins2769284/Figure 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2769284/Figure 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"150420","creation_date":"2024-03-15","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> W+/W- H","H --> A A --> BQ BQ BQ BQ"]},"date":"15 Mar 2024","doc_type":"datatable","doi":"10.17182/hepdata.147309.v1/t1","first_author":{"affiliation":"Yerevan Phys. 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The spectrum is shown in Figure 1 (left panel).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2601274/Table 3 - Away/csv","json":"https://www.hepdata.net/download/table/ins2601274/Table 3 - Away/json","root":"https://www.hepdata.net/download/table/ins2601274/Table 3 - Away/root","yaml":"https://www.hepdata.net/download/table/ins2601274/Table 3 - Away/yaml","yoda":"https://www.hepdata.net/download/table/ins2601274/Table 3 - Away/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"150410","creation_date":"2022-11-28","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["PT"],"phrases":["jets","azimuthal regions","coalescence"],"reactions":["P P --> d X"]},"date":"28 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.141173.v2/t3","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, Shreyasi"},"id":150410,"inspire_id":"2601274","journal_info":"Phys.Rev.Lett. 131 (2023) 042301","keywords":[{"name":"reactions","synonyms":"","value":"P P --> d X"},{"name":"observables","synonyms":"","value":"PT"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"coalescence"},{"name":"phrases","synonyms":"","value":"jets"},{"name":"phrases","synonyms":"","value":"azimuthal regions"}],"last_updated":"2024-03-19T17:00:31","parent_child_join":{"name":"child_datatable","parent":"141173"},"recid":150410,"related_publication":141173,"title":"Table 3 - Away","uuid":"f8fa12df-73bb-4e8c-9884-2f37da31c3b1"},{"abstract":"Transverse momentum spectra for the jet region, obtained as toward-transverse. Events with a leading track with PT>5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (right panel).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2601274/Table 4 - Jet/csv","json":"https://www.hepdata.net/download/table/ins2601274/Table 4 - Jet/json","root":"https://www.hepdata.net/download/table/ins2601274/Table 4 - Jet/root","yaml":"https://www.hepdata.net/download/table/ins2601274/Table 4 - Jet/yaml","yoda":"https://www.hepdata.net/download/table/ins2601274/Table 4 - Jet/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"150411","creation_date":"2022-11-28","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["PT"],"phrases":["jets","azimuthal regions","coalescence"],"reactions":["P P --> d X"]},"date":"28 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.141173.v2/t4","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, Shreyasi"},"id":150411,"inspire_id":"2601274","journal_info":"Phys.Rev.Lett. 131 (2023) 042301","keywords":[{"name":"reactions","synonyms":"","value":"P P --> d X"},{"name":"observables","synonyms":"","value":"PT"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"coalescence"},{"name":"phrases","synonyms":"","value":"jets"},{"name":"phrases","synonyms":"","value":"azimuthal regions"}],"last_updated":"2024-03-19T17:00:31","parent_child_join":{"name":"child_datatable","parent":"141173"},"recid":150411,"related_publication":141173,"title":"Table 4 - Jet","uuid":"c059514b-ddbd-4645-9fb9-d83368c213f4"},{"abstract":"Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the underlying event (transverse region). Events with a leading track with PT>5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2601274/Table 5 - B2 in UE/csv","json":"https://www.hepdata.net/download/table/ins2601274/Table 5 - B2 in UE/json","root":"https://www.hepdata.net/download/table/ins2601274/Table 5 - B2 in UE/root","yaml":"https://www.hepdata.net/download/table/ins2601274/Table 5 - B2 in UE/yaml","yoda":"https://www.hepdata.net/download/table/ins2601274/Table 5 - B2 in UE/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"150412","creation_date":"2022-11-28","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["B2"],"phrases":["jets","azimuthal regions","coalescence"],"reactions":["P P --> d X"]},"date":"28 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.141173.v2/t5","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, Shreyasi"},"id":150412,"inspire_id":"2601274","journal_info":"Phys.Rev.Lett. 131 (2023) 042301","keywords":[{"name":"reactions","synonyms":"","value":"P P --> d X"},{"name":"observables","synonyms":"","value":"B2"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"coalescence"},{"name":"phrases","synonyms":"","value":"jets"},{"name":"phrases","synonyms":"","value":"azimuthal regions"}],"last_updated":"2024-03-19T17:00:31","parent_child_join":{"name":"child_datatable","parent":"141173"},"recid":150412,"related_publication":141173,"title":"Table 5 - B2 in UE","uuid":"e9cd7e62-adf2-475f-ae19-5cdaf61cf7f0"},{"abstract":"Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the jet (transverse-toward region). Events with a leading track with PT>5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2601274/Table 6 - B2 in Jet/csv","json":"https://www.hepdata.net/download/table/ins2601274/Table 6 - B2 in Jet/json","root":"https://www.hepdata.net/download/table/ins2601274/Table 6 - B2 in Jet/root","yaml":"https://www.hepdata.net/download/table/ins2601274/Table 6 - B2 in Jet/yaml","yoda":"https://www.hepdata.net/download/table/ins2601274/Table 6 - B2 in Jet/yoda"}},"authors":null,"collaborations":["ALICE"],"control_number":"150413","creation_date":"2022-11-28","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["B2"],"phrases":["jets","azimuthal regions","coalescence"],"reactions":["P P --> d X"]},"date":"28 Nov 2022","doc_type":"datatable","doi":"10.17182/hepdata.141173.v2/t6","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, Shreyasi"},"id":150413,"inspire_id":"2601274","journal_info":"Phys.Rev.Lett. 131 (2023) 042301","keywords":[{"name":"reactions","synonyms":"","value":"P P --> d X"},{"name":"observables","synonyms":"","value":"B2"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"coalescence"},{"name":"phrases","synonyms":"","value":"jets"},{"name":"phrases","synonyms":"","value":"azimuthal regions"}],"last_updated":"2024-03-19T17:00:31","parent_child_join":{"name":"child_datatable","parent":"141173"},"recid":150413,"related_publication":141173,"title":"Table 6 - B2 in Jet","uuid":"c91c3d40-3a8e-4028-b821-44077c08dfea"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["PT","B2"],"phrases":["jets","azimuthal regions","coalescence"],"reactions":["P P --> d X"]},"date":"28 Nov 2022","doc_type":"publication","doi":"10.1103/PhysRevLett.131.042301","first_author":{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, Shreyasi"},"hepdata_doi":"10.17182/hepdata.141173","id":141173,"inspire_id":"2601274","journal_info":"Phys.Rev.Lett. 131 (2023) 042301","keywords":[{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"deuteron: production"},{"schema":"INSPIRE","value":"model: production"},{"schema":"INSPIRE","value":"model: coalescence"},{"schema":"INSPIRE","value":"cross section: energy dependence"},{"schema":"INSPIRE","value":"jet: fragmentation"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"nucleon"},{"schema":"INSPIRE","value":"underlying event"},{"schema":"INSPIRE","value":"PYTHIA"},{"schema":"INSPIRE","value":"phase space"},{"schema":"INSPIRE","value":"GeV"},{"schema":"INSPIRE","value":"nuclear reaction"},{"schema":"INSPIRE","value":"transverse momentum: momentum spectrum"},{"schema":"INSPIRE","value":"transverse momentum"},{"schema":"INSPIRE","value":"transverse"},{"schema":"INSPIRE","value":"leading particle"},{"schema":"INSPIRE","value":"numerical calculations: Monte Carlo"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"},{"schema":"INSPIRE","value":"TeV"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"numerical calculations"},{"schema":"INSPIRE","value":"pi"},{"schema":"INSPIRE","value":"ALICE"}],"last_updated":"2024-03-19T17:00:32","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-03-19T00:00:00","recid":141173,"subject_area":["hep-ex","nucl-ex"],"summary_authors":[{"affiliation":"Clermont-Ferrand U.","full_name":"Acharya, Shreyasi"},{"affiliation":"Rez, Nucl. 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