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Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2724506/1/csv","json":"https://www.hepdata.net/download/submission/ins2724506/1/json","root":"https://www.hepdata.net/download/submission/ins2724506/1/root","yaml":"https://www.hepdata.net/download/submission/ins2724506/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2724506/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2311.11370","authors":["Tumasyan, Armen","Adam, Wolfgang","Andrejkovic, Janik Walter","Bergauer, Thomas","Chatterjee, Suman","Damanakis, Konstantinos","Dragicevic, Marko","Escalante Del Valle, Alberto","Hussain, Priya Sajid","Jeitler, Manfred"],"collaborations":["CMS"],"control_number":"132638","creation_date":"2023-11-19","data":[{"abstract":"The $v_2\\{2k\\}$ ($k = 1, ..., 5$) values as functions of centrality in PbPb collisions at $\\sqrt{s_{NN}}=5.02~\\textrm{Te}\\textrm{V}$. 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The measurement is performed with charged particles within the acceptance region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2724506/Figure 4/csv","json":"https://www.hepdata.net/download/table/ins2724506/Figure 4/json","root":"https://www.hepdata.net/download/table/ins2724506/Figure 4/root","yaml":"https://www.hepdata.net/download/table/ins2724506/Figure 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2724506/Figure 4/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"147210","creation_date":"2023-11-19","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["Elliptic Flow"],"phrases":["Superskewness","Anisotropic Collective Flow","Skewness","CMS","Kurtosis"],"reactions":["PB PB --> CHARGED X"]},"date":"19 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.132638.v1/t3","first_author":{"affiliation":"Yerevan Phys. 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The measurement is performed with charged particles within the acceptance region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (left)/csv","json":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (left)/json","root":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (left)/root","yaml":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (left)/yaml","yoda":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (left)/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"147211","creation_date":"2023-11-19","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["Elliptic Flow"],"phrases":["Superskewness","Anisotropic Collective Flow","Skewness","CMS","Kurtosis"],"reactions":["PB PB --> CHARGED X"]},"date":"19 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.132638.v1/t4","first_author":{"affiliation":"Yerevan Phys. 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The ratios are plotted as functions of centrality in PbPb collisions at $\\sqrt{s_{NN}}=5.02~\\textrm{Te}\\textrm{V}$. The measurement is performed with charged particles within the acceptance region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (right)/csv","json":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (right)/json","root":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (right)/root","yaml":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (right)/yaml","yoda":"https://www.hepdata.net/download/table/ins2724506/Figure 5 (right)/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"147212","creation_date":"2023-11-19","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["Elliptic Flow"],"phrases":["Superskewness","Anisotropic Collective Flow","Skewness","CMS","Kurtosis"],"reactions":["PB PB --> CHARGED X"]},"date":"19 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.132638.v1/t5","first_author":{"affiliation":"Yerevan Phys. 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The measurement is performed with charged particles within the acceptance region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2724506/Figure 6 (upper)/csv","json":"https://www.hepdata.net/download/table/ins2724506/Figure 6 (upper)/json","root":"https://www.hepdata.net/download/table/ins2724506/Figure 6 (upper)/root","yaml":"https://www.hepdata.net/download/table/ins2724506/Figure 6 (upper)/yaml","yoda":"https://www.hepdata.net/download/table/ins2724506/Figure 6 (upper)/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"147213","creation_date":"2023-11-19","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["Elliptic Flow"],"phrases":["Superskewness","Anisotropic Collective Flow","Skewness","CMS","Kurtosis"],"reactions":["PB PB --> CHARGED X"]},"date":"19 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.132638.v1/t6","first_author":{"affiliation":"Yerevan Phys. 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This analysis is based on proton-proton collision data recorded at $\\sqrt{s}=13$ TeV with the ATLAS detector at the Large Hadron Collider between 2015 and 2018, corresponding to an integrated luminosity of 139 fb$^{-1}$. After selecting events containing large-radius jets with high track multiplicity, the invariant mass distribution of the two highest-transverse-momentum jets is scanned to look for an excess above a data-driven estimate of the Standard Model multijet background. No significant excess of events is observed and the results are thus used to set 95 % confidence-level upper limits on the production cross-section times branching ratio of the $Z^\\prime$ to dark quarks as a function of the $Z^\\prime$ mass for various dark-quark scenarios.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2719976/1/csv","json":"https://www.hepdata.net/download/submission/ins2719976/1/json","root":"https://www.hepdata.net/download/submission/ins2719976/1/root","yaml":"https://www.hepdata.net/download/submission/ins2719976/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2719976/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2311.03944","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"145191","creation_date":"2023-11-07","data":[{"abstract":"Distribution of the di-jet invariant mass, $m_{\\mathrm{JJ}}$ for the data, the simulated multi-jet background and of some representative signals (models A, B, C and D with $m_{Z'}=2.5$ TeV), shown after applying the preselections described in the text. 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In the theory model, a universal coupling of the $Z^\\prime$ to each SM quark $g_q$ is assumed and the dark quarks are all represented by one species with an effective coupling $g_{q_d}$ to the $Z^\\prime$. For model D, the predicted cross-section is shown for $g_q=0.05$ and $g_{q_d} = 0.2$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/csv","json":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/json","root":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Theory cross-section times branching ratio (model D)/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149505","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149505,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149505,"related_publication":145191,"title":"Theory cross-section times branching ratio (model D)","uuid":"fbf552b6-2257-48f4-9399-d25a5efae45f"},{"abstract":"Relative efficiency (in %) of each stage of the analysis selection with respect to the previous one for models A through D and $m_{Z^\\prime}=2.5$ TeV. Approximately 90000 events were generated per signal mass hypothesis.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/csv","json":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/json","root":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/root","yaml":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/yaml","yoda":"https://www.hepdata.net/download/table/ins2719976/Cutflow table for signal points/yoda"}},"authors":null,"collaborations":["ATLAS"],"control_number":"149506","creation_date":"2023-11-07","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["EFF"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"datatable","doi":"10.17182/hepdata.145191.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":149506,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"observables","synonyms":"","value":"EFF"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"}],"last_updated":"2024-02-23T16:19:59","parent_child_join":{"name":"child_datatable","parent":"145191"},"recid":149506,"related_publication":145191,"title":"Cutflow table for signal points","uuid":"eec313ce-c239-4f90-82ab-0611cde4ec81"}],"data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["CLS","M","EFF"],"phrases":["Proton-Proton Scattering"],"reactions":["P P --> ZPRIME"]},"date":"07 Nov 2023","doc_type":"publication","doi":"10.1007/JHEP02(2024)128","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.145191","id":145191,"inspire_id":"2719976","journal_info":"JHEP 02 (2024) 128","keywords":[{"source":"author","value":"Beyond Standard Model"},{"source":"author","value":"Hadron-Hadron Scattering"},{"source":"author","value":"Dark Matter"},{"source":"author","value":"Exotics"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"jet: pair production"},{"schema":"INSPIRE","value":"resonance: production"},{"schema":"INSPIRE","value":"tracks: multiplicity"},{"schema":"INSPIRE","value":"multiplicity: high"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"jet: multiple production"},{"schema":"INSPIRE","value":"dijet: final state"},{"schema":"INSPIRE","value":"final state: ((n)jet)"},{"schema":"INSPIRE","value":"quark"},{"schema":"INSPIRE","value":"hidden sector"},{"schema":"INSPIRE","value":"ATLAS"},{"schema":"INSPIRE","value":"channel cross section: branching ratio: upper limit"},{"schema":"INSPIRE","value":"mass dependence"},{"schema":"INSPIRE","value":"Z': mass"},{"schema":"INSPIRE","value":"Z': hadronic decay"},{"schema":"INSPIRE","value":"dijet: mass spectrum"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"background"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2024-02-23T16:20:01","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-03-21T00:00:00","recid":145191,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"Gottingen U., II. Phys. Inst.","full_name":"Abeling, Kira"},{"affiliation":"Dortmund U.","full_name":"Abicht, Nils Julius"},{"affiliation":"Brookhaven","full_name":"Abidi, Haider"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"},{"affiliation":"Technion","full_name":"Abreu, Henso"},{"affiliation":"New York U.","full_name":"Abulaiti, Yiming"},{"affiliation":"INFN, Udine","full_name":"Acharya, Bobby Samir"}],"title":"Search for Resonant Production of Dark Quarks in the Dijet Final State with the ATLAS Detector","total_tables":13,"type":["article"],"uuid":"f232ecd8-3971-4045-98d2-fee1f5ff0918","version":1,"year":"2024"},{"abstract":"A search for a heavy CP-odd Higgs boson, $A$, decaying into a $Z$ boson and a heavy CP-even Higgs boson, $H$, is presented. It uses the full LHC Run 2 dataset of $pp$ collisions at $\\sqrt{s}=13$ TeV collected with the ATLAS detector, corresponding to an integrated luminosity of $140$ fb$^{-1}$. The search for $A\\to ZH$ is performed in the $\\ell^+\\ell^- t\\bar{t}$ and $\\nu\\bar{\\nu}b\\bar{b}$ final states and surpasses the reach of previous searches in different final states in the region with $m_H>350$ GeV and $m_A>800$ GeV. No significant deviation from the Standard Model expectation is found. Upper limits are placed on the production cross-section times the decay branching ratios. Limits with less model dependence are also presented as functions of the reconstructed $m(t\\bar{t})$ and $m(b\\bar{b})$ distributions in the $\\ell^+\\ell^- t\\bar{t}$ and $\\nu\\bar{\\nu}b\\bar{b}$ channels, respectively. In addition, the results are interpreted in the context of two-Higgs-doublet models.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2719822/1/csv","json":"https://www.hepdata.net/download/submission/ins2719822/1/json","root":"https://www.hepdata.net/download/submission/ins2719822/1/root","yaml":"https://www.hepdata.net/download/submission/ins2719822/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2719822/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2311.04033","authors":["Aad, Georges","Abbott, Braden Keim","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboulhorma, Asmaa","Abramowicz, Halina","Abreu, Henso","Abulaiti, Yiming","Acharya, Bobby Samir"],"collaborations":["ATLAS"],"control_number":"144335","creation_date":"2023-11-07","data":[{"abstract":"Overview of HEPData Record
\nUpper limits on cross-sections:\n