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The error bands include both the statistical and systematic uncertainties.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 3a/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 3a/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 3a/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 3a/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 3a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 3a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168531","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168531,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168531,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160345?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160346?landing_page=true"}],"title":"Figure 3a","uuid":"48e735e5-0bb0-4fcf-b684-7867e877a7f3"},{"abstract":"Post-fit distributions of the reconstructed m<sub>t&#772;t</sub> for the three signal regions of the 1-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Vjets&quot; refers to the Z + jets and W+ jets backgrounds, whilst &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR1b resolved)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR1b resolved)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR1b resolved)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR1b resolved)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR1b resolved)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR1b resolved)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168532","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168532,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168532,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160348?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160349?landing_page=true"}],"title":"Figure 6 (SR1b resolved)","uuid":"e01660ed-a4ca-47b9-8199-3f5b283bfca2"},{"abstract":"Post-fit distributions of the reconstructed m<sub>t&#772;t</sub> for the three signal regions of the 1-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Vjets&quot; refers to the Z + jets and W+ jets backgrounds, whilst &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR2b resolved)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR2b resolved)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR2b resolved)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR2b resolved)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR2b resolved)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR2b resolved)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168533","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168533,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168533,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160351?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160352?landing_page=true"}],"title":"Figure 6 (SR2b resolved)","uuid":"5d1ca45a-863e-4da5-b42b-eab3e52f1242"},{"abstract":"Post-fit distributions of the reconstructed m<sub>t&#772;t</sub> for the three signal regions of the 1-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Vjets&quot; refers to the Z + jets and W+ jets backgrounds, whilst &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR merged)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR merged)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR merged)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR merged)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR merged)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 6 (SR merged)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168534","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168534,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168534,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160354?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160355?landing_page=true"}],"title":"Figure 6 (SR merged)","uuid":"a9c1eeb9-f332-4d67-897b-7d7932d9ae60"},{"abstract":"Post-fit distributions of the reconstructed m<sub>llbb</sub> for the five signal regions of the 2-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR1)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR1)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR1)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR1)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR1)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR1)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168535","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168535,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168535,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160357?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160358?landing_page=true"}],"title":"Figure 7 (SR1)","uuid":"76d0e652-d8af-4041-a75f-a839269d43d5"},{"abstract":"Post-fit distributions of the reconstructed m<sub>llbb</sub> for the five signal regions of the 2-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR2)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR2)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR2)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR2)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR2)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR2)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168536","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168536,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168536,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160360?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160361?landing_page=true"}],"title":"Figure 7 (SR2)","uuid":"b034e74f-ea0d-40d3-9348-561752c06319"},{"abstract":"Post-fit distributions of the reconstructed m<sub>llbb</sub> for the five signal regions of the 2-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR3)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR3)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR3)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR3)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR3)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR3)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168537","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168537,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168537,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160363?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160364?landing_page=true"}],"title":"Figure 7 (SR3)","uuid":"b9458a21-fc1f-48d7-ac8e-9fbbf2b87f93"},{"abstract":"Post-fit distributions of the reconstructed m<sub>llbb</sub> for the five signal regions of the 2-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR4)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR4)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR4)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR4)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR4)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR4)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168538","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168538,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168538,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160366?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160367?landing_page=true"}],"title":"Figure 7 (SR4)","uuid":"6fe0ccc6-6237-4c05-bad6-371195cebb40"},{"abstract":"Post-fit distributions of the reconstructed m<sub>llbb</sub> for the five signal regions of the 2-lepton channel, after performing the profile-likelihood fit under the background-only hypothesis in the 3+5 signal regions of the 1-lepton and 2-lepton channels, respectively. The overflow is added to the final bins. The lower panel shows the pulls from the fit (red line), where the pull in each bin is defined as (n<sub>obs</sub>-n<sub>pred</sub>)/&radic;n<sub>obs</sub>, and n<sub>obs</sub> and n<sub>pred</sub> refer to the number of observed events in data and the number of predicted events, respectively. &quot;Other Bkg.&quot; combines the t&#772;t + V, t&#772;t + H, diboson, and fakes backgrounds together.\n\nThe table below shows the total number of events in each bin, and is not normalised by bin width.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR5)/csv","json":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR5)/json","root":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR5)/root","yaml":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR5)/yaml","yoda":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR5)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3094414/Figure 7 (SR5)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168539","creation_date":"2025-12-19","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"datatable","doi":"10.17182/hepdata.168229.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168539,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Graviton"},{"name":"phrases","synonyms":"","value":"Z'"},{"name":"phrases","synonyms":"","value":"tt resonance"},{"name":"reactions","synonyms":"","value":"pp -> Z' -> tt"}],"last_updated":"2026-02-12T21:50:04","parent_child_join":{"name":"child_datatable","parent":"168229"},"recid":168539,"related_publication":168229,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4160369?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4160370?landing_page=true"}],"title":"Figure 7 (SR5)","uuid":"0c53ca21-867d-41e6-a897-7c307f74dc49"},{"abstract":"Observed (pink data points) and expected (black dashed line) upper limits on the signal cross-section times branching ratio to tt&#772; for the (a) Z', (b) G<sub>KK</sub>, and (c) g<sub>KK</sub> signals at 95&percnt; CL. 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Final states with either exactly one electron or muon, or exactly two leptons ($ee$, $\\mu\\mu$ or $e\\mu$), large missing transverse momentum, and two jets, at least one of which must be identified as likely containing a b-hadron decay, are considered. The search targets resonances with both narrow and broad widths relative to the detector resolution, and with masses in the range of 0.4-5.0 TeV. No significant deviation from the Standard Model prediction is observed. Exclusion limits are set on the production cross-section times branching ratio for hypothetical $Z'$ bosons, Kaluza\u2013Klein gravitons, and Kaluza\u2013Klein gluons that decay into top-quark pairs.","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["tt resonance","Z'","Graviton"],"reactions":["pp -> Z' -> tt"]},"date":"19 Dec 2025","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.168229","id":168229,"inspire_id":"3094414","journal_info":"CERN-EP-2025-281","keywords":[],"last_updated":"2026-02-12T21:50:07","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-02-12T00:00:00","recid":168229,"resources":[{"description":"Created with hepdata_lib 0.20.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"Webpage with all figures and tables","type":"html","url":"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2018-49/"},{"description":"arXiv","type":"html","url":"https://arxiv.org/abs/2512.17856"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"New York U., Abu Dhabi","full_name":"Abdelhameed, Sara"},{"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":"Southern Methodist U.","full_name":"Aboelela, Mohammed"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"}],"title":"Search for ttbar resonances in final states with exactly one or two leptons using 140 fb$^{-1}$ of pp collision data at $\\sqrt{s}=13$ TeV with the ATLAS experiment","total_tables":21,"type":["article"],"uuid":"5fbb1252-bf5d-452a-8e6b-a5eb078e8bf1","version":1,"year":"2025"},{"abstract":"A search is presented for emerging jets using 140 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s} = 13$ TeV, collected by the ATLAS experiment between 2015 and 2018. The search looks for the existence of a dark sector with symmetries similar to those in quantum chromodynamics. This dark sector is populated with dark quarks, which undergo showering similar to quarks in the Standard Model, leading to a high multiplicity of long-lived dark hadrons within a dark jet. These dark hadrons subsequently decay to Standard Model particles via a new heavy scalar mediating particle $\u03d5$. This results in jets which contain multiple displaced vertices, known as emerging jets. This analysis targets four-jet topologies, with two emerging jets and two Standard Model jets, resulting from the decay of pair-produced scalar mediators. No significant excess above the Standard Model background is observed. For dark pion proper decay lengths of 20 mm, mediator masses are excluded between 1 TeV and 2 TeV assuming a dark pion mass of 20 GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins3069355/1/csv","json":"https://www.hepdata.net/download/submission/ins3069355/1/json","root":"https://www.hepdata.net/download/submission/ins3069355/1/root","yaml":"https://www.hepdata.net/download/submission/ins3069355/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins3069355/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins3069355/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2510.12347","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abdelhameed, Sara","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboelela, Mohammed","Aboulhorma, Asmaa","Abramowicz, Halina"],"collaborations":["ATLAS"],"control_number":"167179","creation_date":"2025-10-14","data":[{"abstract":"Comparison of the data with N<sub>DV</sub> &gt; 1 and the estimated background in the SR using the modified ABCD method. The division between the SR and CR is shown by the vertical dashed line. In the final fit, the bins with R &gt; 0.4 are combined into a single bin. Three selected signal samples are included for comparison.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3069355/Figure 5/csv","json":"https://www.hepdata.net/download/table/ins3069355/Figure 5/json","root":"https://www.hepdata.net/download/table/ins3069355/Figure 5/root","yaml":"https://www.hepdata.net/download/table/ins3069355/Figure 5/yaml","yoda":"https://www.hepdata.net/download/table/ins3069355/Figure 5/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3069355/Figure 5/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167496","creation_date":"2025-10-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark QCD","Emerging Jets"],"reactions":["pp -> Qd Qd q q"]},"date":"14 Oct 2025","doc_type":"datatable","doi":"10.17182/hepdata.167179.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167496,"inspire_id":"3069355","journal_info":"CERN-EP-2025-225","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark QCD"},{"name":"phrases","synonyms":"","value":"Emerging Jets"},{"name":"reactions","synonyms":"","value":"pp -> Qd Qd q q"}],"last_updated":"2025-12-31T17:30:45","parent_child_join":{"name":"child_datatable","parent":"167179"},"recid":167496,"related_publication":167179,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4066234?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4066235?landing_page=true"}],"title":"Figure 5","uuid":"392101b6-2655-470d-b08c-c461121e036c"},{"abstract":"95&percnt; CL upper limits as a function of (left) c&tau;<sub>&pi;<sub>d</sub></sub> and (right) M<sub>&phi;</sub>. The upper plots show the expected and observed limits on &sigma;(pp &rarr;&phi;<sup>&dagger;</sup>&phi;) for m<sub>&pi;<sub>d</sub></sub> = 20&nbsp;GeV: (a) using M<sub>&phi;</sub> = 1.6&nbsp;TeV and (b) using c&tau;<sub>&pi;<sub>d</sub></sub> = 20&nbsp;mm. The lower plots show a comparison of the observed limits for all three dark pion masses: (c) using M<sub>&phi;</sub> = 1.4&nbsp;TeV, and (d) using c&tau;<sub>&pi;<sub>d</sub></sub> = 1&nbsp;mm. The mediator mass-dependent theoretical cross-section is given with the band corresponding to the uncertainty from NNLL-Fast.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3069355/Figure 6a/csv","json":"https://www.hepdata.net/download/table/ins3069355/Figure 6a/json","root":"https://www.hepdata.net/download/table/ins3069355/Figure 6a/root","yaml":"https://www.hepdata.net/download/table/ins3069355/Figure 6a/yaml","yoda":"https://www.hepdata.net/download/table/ins3069355/Figure 6a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3069355/Figure 6a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167497","creation_date":"2025-10-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark QCD","Emerging Jets"],"reactions":["pp -> Qd Qd q q"]},"date":"14 Oct 2025","doc_type":"datatable","doi":"10.17182/hepdata.167179.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167497,"inspire_id":"3069355","journal_info":"CERN-EP-2025-225","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark QCD"},{"name":"phrases","synonyms":"","value":"Emerging Jets"},{"name":"reactions","synonyms":"","value":"pp -> Qd Qd q q"}],"last_updated":"2025-12-31T17:30:45","parent_child_join":{"name":"child_datatable","parent":"167179"},"recid":167497,"related_publication":167179,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4066237?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4066238?landing_page=true"}],"title":"Figure 6a","uuid":"9c598f8d-9032-4ae7-8b0e-d1593e873269"},{"abstract":"95&percnt; CL upper limits as a function of (left) c&tau;<sub>&pi;<sub>d</sub></sub> and (right) M<sub>&phi;</sub>. The upper plots show the expected and observed limits on &sigma;(pp &rarr;&phi;<sup>&dagger;</sup>&phi;) for m<sub>&pi;<sub>d</sub></sub> = 20&nbsp;GeV: (a) using M<sub>&phi;</sub> = 1.6&nbsp;TeV and (b) using c&tau;<sub>&pi;<sub>d</sub></sub> = 20&nbsp;mm. The lower plots show a comparison of the observed limits for all three dark pion masses: (c) using M<sub>&phi;</sub> = 1.4&nbsp;TeV, and (d) using c&tau;<sub>&pi;<sub>d</sub></sub> = 1&nbsp;mm. The mediator mass-dependent theoretical cross-section is given with the band corresponding to the uncertainty from NNLL-Fast.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3069355/Figure 6b/csv","json":"https://www.hepdata.net/download/table/ins3069355/Figure 6b/json","root":"https://www.hepdata.net/download/table/ins3069355/Figure 6b/root","yaml":"https://www.hepdata.net/download/table/ins3069355/Figure 6b/yaml","yoda":"https://www.hepdata.net/download/table/ins3069355/Figure 6b/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3069355/Figure 6b/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167498","creation_date":"2025-10-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark QCD","Emerging Jets"],"reactions":["pp -> Qd Qd q q"]},"date":"14 Oct 2025","doc_type":"datatable","doi":"10.17182/hepdata.167179.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167498,"inspire_id":"3069355","journal_info":"CERN-EP-2025-225","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark QCD"},{"name":"phrases","synonyms":"","value":"Emerging Jets"},{"name":"reactions","synonyms":"","value":"pp -> Qd Qd q q"}],"last_updated":"2025-12-31T17:30:45","parent_child_join":{"name":"child_datatable","parent":"167179"},"recid":167498,"related_publication":167179,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4066240?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4066241?landing_page=true"}],"title":"Figure 6b","uuid":"3a13ba08-ca71-40d7-9f71-e23b9e9ab607"},{"abstract":"95&percnt; CL upper limits as a function of (left) c&tau;<sub>&pi;<sub>d</sub></sub> and (right) M<sub>&phi;</sub>. The upper plots show the expected and observed limits on &sigma;(pp &rarr;&phi;<sup>&dagger;</sup>&phi;) for m<sub>&pi;<sub>d</sub></sub> = 20&nbsp;GeV: (a) using M<sub>&phi;</sub> = 1.6&nbsp;TeV and (b) using c&tau;<sub>&pi;<sub>d</sub></sub> = 20&nbsp;mm. The lower plots show a comparison of the observed limits for all three dark pion masses: (c) using M<sub>&phi;</sub> = 1.4&nbsp;TeV, and (d) using c&tau;<sub>&pi;<sub>d</sub></sub> = 1&nbsp;mm. The mediator mass-dependent theoretical cross-section is given with the band corresponding to the uncertainty from NNLL-Fast.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3069355/Figure 6c/csv","json":"https://www.hepdata.net/download/table/ins3069355/Figure 6c/json","root":"https://www.hepdata.net/download/table/ins3069355/Figure 6c/root","yaml":"https://www.hepdata.net/download/table/ins3069355/Figure 6c/yaml","yoda":"https://www.hepdata.net/download/table/ins3069355/Figure 6c/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3069355/Figure 6c/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167499","creation_date":"2025-10-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark QCD","Emerging Jets"],"reactions":["pp -> Qd Qd q q"]},"date":"14 Oct 2025","doc_type":"datatable","doi":"10.17182/hepdata.167179.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167499,"inspire_id":"3069355","journal_info":"CERN-EP-2025-225","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark QCD"},{"name":"phrases","synonyms":"","value":"Emerging Jets"},{"name":"reactions","synonyms":"","value":"pp -> Qd Qd q q"}],"last_updated":"2025-12-31T17:30:45","parent_child_join":{"name":"child_datatable","parent":"167179"},"recid":167499,"related_publication":167179,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4066243?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4066244?landing_page=true"}],"title":"Figure 6c","uuid":"dca0330b-412d-446b-bd5e-2792618833cf"},{"abstract":"95&percnt; CL upper limits as a function of (left) c&tau;<sub>&pi;<sub>d</sub></sub> and (right) M<sub>&phi;</sub>. The upper plots show the expected and observed limits on &sigma;(pp &rarr;&phi;<sup>&dagger;</sup>&phi;) for m<sub>&pi;<sub>d</sub></sub> = 20&nbsp;GeV: (a) using M<sub>&phi;</sub> = 1.6&nbsp;TeV and (b) using c&tau;<sub>&pi;<sub>d</sub></sub> = 20&nbsp;mm. The lower plots show a comparison of the observed limits for all three dark pion masses: (c) using M<sub>&phi;</sub> = 1.4&nbsp;TeV, and (d) using c&tau;<sub>&pi;<sub>d</sub></sub> = 1&nbsp;mm. The mediator mass-dependent theoretical cross-section is given with the band corresponding to the uncertainty from NNLL-Fast.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3069355/Figure 6d/csv","json":"https://www.hepdata.net/download/table/ins3069355/Figure 6d/json","root":"https://www.hepdata.net/download/table/ins3069355/Figure 6d/root","yaml":"https://www.hepdata.net/download/table/ins3069355/Figure 6d/yaml","yoda":"https://www.hepdata.net/download/table/ins3069355/Figure 6d/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3069355/Figure 6d/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167500","creation_date":"2025-10-14","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Dark QCD","Emerging Jets"],"reactions":["pp -> Qd Qd q q"]},"date":"14 Oct 2025","doc_type":"datatable","doi":"10.17182/hepdata.167179.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167500,"inspire_id":"3069355","journal_info":"CERN-EP-2025-225","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Dark QCD"},{"name":"phrases","synonyms":"","value":"Emerging Jets"},{"name":"reactions","synonyms":"","value":"pp -> Qd Qd q q"}],"last_updated":"2025-12-31T17:30:45","parent_child_join":{"name":"child_datatable","parent":"167179"},"recid":167500,"related_publication":167179,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4066246?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4066247?landing_page=true"}],"title":"Figure 6d","uuid":"671def9e-e6e4-4f8b-9e84-6e52ba145b87"},{"abstract":"95&percnt; CL exclusion contours as a function of M<sub>&phi;</sub> and c&tau;<sub>&pi;<sub>d</sub></sub>. The expected and observed limits on &sigma;(pp &rarr;&phi;<sup>&dagger;</sup>&phi;) are shown for (a) m<sub>&pi;<sub>d</sub></sub> = 5&nbsp;GeV, (b) m<sub>&pi;<sub>d</sub></sub> = 10&nbsp;GeV, and (c) m<sub>&pi;<sub>d</sub></sub> = 20&nbsp;GeV. 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This paper presents for the first time the measurement of the full set of angular coefficients together with the differential cross-section as a function of the transverse momentum of the $W$ boson, in the full phase space of the decay leptons. The measurements are performed separately for the W<sup>-</sup> and W<sup>+</sup> channels.The analysis uses proton proton collision data recorded by the ATLAS experiment at the Large Hadron Collider in 2017 and 2018, during special low-luminosity runs with a reduced number of interactions per bunch crossings (pile-up). The data correspond to an integrated luminosity of 338 pb<sup>-1</sup> at a centre-of-mass energy of &radic;s=13 TeV. The low pile-up conditions enable an optimised reconstruction of the W boson transverse momentum. All results agree with theory predictions incorporating finite-order QCD corrections up to next-to-next-to-leading-order in the strong coupling constant.","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["AI","CORR","$d\\sigma/dp_{T}$"],"phrases":["W Production","Transverse Momentum Dependence","Inclusive","Single Differential Distribution","Proton-Proton Scattering"],"reactions":["P P --> W+ --> l+ nu","P P --> W- --> l- nu"]},"date":"17 Sep 2025","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.166079","id":166079,"inspire_id":"2970689","journal_info":"CERN-EP-2025-188","keywords":[],"last_updated":"2026-01-08T11:33:23","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-01-08T00:00:00","recid":166079,"resources":[{"description":"Created with hepdata_lib 0.20.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"Webpage with all figures and tables","type":"html","url":"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/STDM-2020-07/"},{"description":"arXiv","type":"html","url":"https://arxiv.org/abs/2509.13759"},{"description":"Original abstract file","type":"Text","url":"https://www.hepdata.net/record/resource/3998504?landing_page=true"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"New York U., Abu Dhabi","full_name":"Abdelhameed, Sara"},{"affiliation":"Gottingen U., II. 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The $v_{n}$ coefficients are measured as a function of transverse momentum ($p_{\\mathrm{T}}$), collision centrality, and event multiplicity. They are extracted using two complementary methods: two-particle correlations with a template-fit subtraction of short-range non-flow contributions, and four-particle subevent cumulants, which intrinsically suppress non-flow effects and provide sensitivity to flow fluctuations. The results show a clear hierarchy $v_{2} > v_{3} > v_{4}$ and a non-monotonic dependence on $p_{\\mathrm{T}}$, reaching a maximum around 2 GeV, consistent with trends observed in heavy-ion collisions. Detailed comparisons between the two collision systems reveal an enhanced $v_{2}$ in central $\\mathrm{^{20}Ne}+\\mathrm{^{20}Ne}$ collisions, consistent with theory expectations based on the predicted prolate deformation of neon nuclei, in contrast to the slightly tetrahedral structure predicted for oxygen. The four-particle cumulant results highlight strong event-by-event fluctuations and provide the greatest sensitivity to nuclear shape effects. 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The vertical lines and vertical bars indicate statistical and systematic uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2967110/Figure 5f (2)/csv","json":"https://www.hepdata.net/download/table/ins2967110/Figure 5f (2)/json","root":"https://www.hepdata.net/download/table/ins2967110/Figure 5f (2)/root","yaml":"https://www.hepdata.net/download/table/ins2967110/Figure 5f (2)/yaml","yoda":"https://www.hepdata.net/download/table/ins2967110/Figure 5f (2)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2967110/Figure 5f (2)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168800","creation_date":"2025-09-05","data_keywords":{"cmenergies":[{"gte":5360.0,"lte":5360.0}],"phrases":["azimuthal anisotropy","charged particles"],"reactions":["NE NE --> CHARGED X","O O --> CHARGED X"]},"date":"05 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.168010.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168800,"inspire_id":"2967110","journal_info":"CERN-EP-2025-200","keywords":[{"name":"cmenergies","synonyms":"","value":"5360"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"charged particles"},{"name":"reactions","synonyms":"","value":"O O --> CHARGED X"},{"name":"reactions","synonyms":"","value":"NE NE --> CHARGED X"}],"last_updated":"2026-02-24T08:41:25","parent_child_join":{"name":"child_datatable","parent":"168010"},"recid":168800,"related_publication":168010,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4166261?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4166262?landing_page=true"}],"title":"Figure 5f (2)","uuid":"11d67ffd-e3ad-469d-82c3-e150aa449161"},{"abstract":"The p<sub>T</sub><sup>b</sup> dependence of the v<sub>n</sub><sup>2PC</sup>{2} and v<sub>n</sub><sup>sub</sup>{2} in the (a,&nbsp;c,&nbsp;e) O+O and (b,&nbsp;d,&nbsp;f) Ne+Ne collisions, for the (a,&nbsp;b) 0&ndash;5&percnt;, (c,&nbsp;d) 20&ndash;30&percnt; and (e,&nbsp;f) 50&ndash;60&percnt; centrality intervals. 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The Ne+Ne points are slightly displaced along the horizontal axis for visual clarity. (b) Ratios of the flow coefficients in Ne+Ne to those in O+O collisions, corresponding to the results in panel (a). Ratios are shown only for the 0&ndash;50&percnt; centrality range to suppress large statistical fluctuations in more peripheral intervals. The vertical lines and vertical bars indicate statistical and systematic uncertainties, respectively. 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The Ne+Ne points are slightly displaced along the horizontal axis for visual clarity. (b) Ratios of the flow coefficients in Ne+Ne to those in O+O collisions, corresponding to the results in panel (a). Ratios are shown only for the 0&ndash;50&percnt; centrality range to suppress large statistical fluctuations in more peripheral intervals. The vertical lines and vertical bars indicate statistical and systematic uncertainties, respectively. 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The Ne+Ne points are slightly displaced along the horizontal axis for visual clarity. (b) Ratios of the flow coefficients in Ne+Ne to those in O+O collisions, corresponding to the results in panel (a). Ratios are shown only for the 0&ndash;50&percnt; centrality range to suppress large statistical fluctuations in more peripheral intervals. The vertical lines and vertical bars indicate statistical and systematic uncertainties, respectively. 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The Ne+Ne points are slightly displaced along the horizontal axis for visual clarity. (b) Ratios of the flow coefficients in Ne+Ne to those in O+O collisions, corresponding to the results in panel (a). Ratios are shown only for the 0&ndash;50&percnt; centrality range to suppress large statistical fluctuations in more peripheral intervals. The vertical lines and vertical bars indicate statistical and systematic uncertainties, respectively. 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The Ne+Ne points are slightly displaced along the horizontal axis for visual clarity. (b) Ratios of the flow coefficients in Ne+Ne to those in O+O collisions, corresponding to the results in panel (a). The vertical lines and vertical bars indicate statistical and systematic uncertainties, respectively. 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Panel (a) is identical to Figure&nbsp;5b.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2967110/Figure 2h from Auxiliary material (3)/csv","json":"https://www.hepdata.net/download/table/ins2967110/Figure 2h from Auxiliary material (3)/json","root":"https://www.hepdata.net/download/table/ins2967110/Figure 2h from Auxiliary material (3)/root","yaml":"https://www.hepdata.net/download/table/ins2967110/Figure 2h from Auxiliary material (3)/yaml","yoda":"https://www.hepdata.net/download/table/ins2967110/Figure 2h from Auxiliary material (3)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2967110/Figure 2h from Auxiliary material (3)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"168853","creation_date":"2025-09-05","data_keywords":{"cmenergies":[{"gte":5360.0,"lte":5360.0}],"phrases":["azimuthal anisotropy","charged particles"],"reactions":["NE NE --> CHARGED X","O O --> CHARGED X"]},"date":"05 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.168010.v1/t67","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":168853,"inspire_id":"2967110","journal_info":"CERN-EP-2025-200","keywords":[{"name":"cmenergies","synonyms":"","value":"5360"},{"name":"phrases","synonyms":"","value":"azimuthal anisotropy"},{"name":"phrases","synonyms":"","value":"charged particles"},{"name":"reactions","synonyms":"","value":"O O --> CHARGED X"},{"name":"reactions","synonyms":"","value":"NE NE --> CHARGED X"}],"last_updated":"2026-02-24T08:41:25","parent_child_join":{"name":"child_datatable","parent":"168010"},"recid":168853,"related_publication":168010,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4166420?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4166421?landing_page=true"}],"title":"Figure 2h from Auxiliary material (3)","uuid":"4dbdad8b-3e68-4f3e-b557-c2680f2bee74"}],"data_abstract":"This paper presents the first measurements of the azimuthal anisotropy    coefficients $v_{n}$, which quantify the $n^{\\mathrm{th}}$-order    Fourier modulation of charged-particle azimuthal distributions,    for $n=2$-4 in $\\sqrt{s_{\\mathrm{NN}}}=5.36$ TeV    $\\mathrm{^{16}O}+\\mathrm{^{16}O}$ and $\\mathrm{^{20}Ne}+\\mathrm{^{20}Ne}$    collisions recorded with the ATLAS detector at the Large Hadron Collider in 2025.  The $v_{n}$ coefficients are measured as a function of transverse momentum ($p_{\\mathrm{T}}$),    collision centrality, and event multiplicity.  They are extracted using two complementary methods: two-particle correlations    with a template-fit subtraction of short-range non-flow contributions,    and four-particle subevent cumulants, which intrinsically suppress non-flow    effects and provide sensitivity to flow fluctuations.  The results show a clear hierarchy $v_{2} > v_{3} > v_{4}$ and a non-monotonic    dependence on $p_{\\mathrm{T}}$, reaching a maximum around 2 GeV, consistent with trends    observed in heavy-ion collisions.  Detailed comparisons between the two collision systems reveal an    enhanced $v_{2}$ in central $\\mathrm{^{20}Ne}+\\mathrm{^{20}Ne}$ collisions,    consistent with theory expectations based on the predicted prolate    deformation of neon nuclei, in contrast to the slightly tetrahedral structure    predicted for oxygen.  The four-particle cumulant results highlight strong event-by-event fluctuations    and provide the greatest sensitivity to nuclear shape effects.  These measurements can place new constraints on the initial geometry and the    hydrodynamic response in light-ion collisions, offering valuable input for    models of nuclear structure.","data_keywords":{"cmenergies":[{"gte":5360.0,"lte":5360.0}],"phrases":["azimuthal anisotropy","charged particles"],"reactions":["NE NE --> CHARGED X","O O --> CHARGED X"]},"date":"05 Sep 2025","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.168010","id":168010,"inspire_id":"2967110","journal_info":"CERN-EP-2025-200","keywords":[],"last_updated":"2026-02-24T08:41:34","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-03-03T00:00:00","recid":168010,"resources":[{"description":"Created with hepdata_lib 0.20.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"Webpage with all figures and tables","type":"html","url":"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HION-2025-02/"},{"description":"arXiv","type":"html","url":"https://arxiv.org/abs/2509.05171"}],"subject_area":["hep-ex","nucl-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"New York U., Abu Dhabi","full_name":"Abdelhameed, Sara"},{"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":"Southern Methodist U.","full_name":"Aboelela, Mohammed"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"}],"title":"Measurement of the azimuthal anisotropy of charged particles in $\\sqrt{s_{\\mathrm{NN}}}=5.36$ TeV $^{16}$O$+^{16}$O and $^{20}$Ne$+^{20}$Ne collisions with the ATLAS detector","total_tables":67,"type":["article"],"uuid":"f65a2dc6-2d4e-4f4b-96ca-82f0024fadc8","version":1,"year":"2025"},{"abstract":"This article reports on a search for dijet resonances using $132$ fb$^{-1}$ of $pp$ collision data recorded at $\\sqrt{s} = 13$ TeV by the ATLAS detector at the Large Hadron Collider. The search is performed solely on jets reconstructed within the ATLAS trigger to overcome bandwidth limitations imposed on conventional single-jet triggers, which would otherwise reject data from decays of sub-TeV dijet resonances. Collision events with two jets satisfying transverse momentum thresholds of $p_{\\textrm{T}} \\ge 85$ GeV and jet rapidity separation of $|y^{*}|<0.6$ are analysed for dijet resonances with invariant masses from $375$ to $1800$ GeV. A data-driven background estimate is used to model the dijet mass distribution from multijet processes. No significant excess above the expected background is observed. Upper limits are set at $95\\%$ confidence level on coupling values for a benchmark leptophobic axial-vector $Z^{\\prime}$ model and on the production cross-section for a new resonance contributing a Gaussian-distributed line-shape to the dijet mass distribution.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2966134/1/csv","json":"https://www.hepdata.net/download/submission/ins2966134/1/json","root":"https://www.hepdata.net/download/submission/ins2966134/1/root","yaml":"https://www.hepdata.net/download/submission/ins2966134/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2966134/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2966134/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2509.01219","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abdelhameed, Sara","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboelela, Mohammed","Aboulhorma, Asmaa","Abramowicz, Halina"],"collaborations":["ATLAS"],"control_number":"161624","creation_date":"2025-09-01","data":[{"abstract":"Observed $m_{jj}$ distribution for the J50 signal region, using variable-width bins and the analysis selections. The background estimate corresponds to the ansatz fit, integrated over each bin.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J50)/csv","json":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J50)/json","root":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J50)/root","yaml":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J50)/yaml","yoda":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J50)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J50)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"165470","creation_date":"2025-09-01","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["P P --> JET JET"],"phrases":["Dijet Production","Trigger-level","Dark Matter","Proton-Proton Scattering","Resonance"],"reactions":["P P --> ZPRIME --> JET JET"]},"date":"01 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.161624.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":165470,"inspire_id":"2966134","journal_info":"Phys.Rev.D 112 (2025) 092015","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Dijet Production"},{"name":"phrases","synonyms":"","value":"Resonance"},{"name":"phrases","synonyms":"","value":"Trigger-level"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME --> JET JET"},{"name":"observables","synonyms":"","value":"P P --> JET JET"}],"last_updated":"2025-09-22T18:12:52","parent_child_join":{"name":"child_datatable","parent":"161624"},"recid":165470,"related_publication":161624,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3965476?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3965477?landing_page=true"}],"title":"Dijet mass distribution (J50)","uuid":"12b2a806-f7eb-4ec2-957c-b48bd5f3f93c"},{"abstract":"Observed $m_{jj}$ distribution for the J100 signal region, using variable-width bins and the analysis selections. The background estimate corresponds to the ansatz fit, integrated over each bin.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J100)/csv","json":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J100)/json","root":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J100)/root","yaml":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J100)/yaml","yoda":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J100)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2966134/Dijet mass distribution (J100)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"165471","creation_date":"2025-09-01","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["P P --> JET JET"],"phrases":["Dijet Production","Trigger-level","Dark Matter","Proton-Proton Scattering","Resonance"],"reactions":["P P --> ZPRIME --> JET JET"]},"date":"01 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.161624.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":165471,"inspire_id":"2966134","journal_info":"Phys.Rev.D 112 (2025) 092015","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Dijet Production"},{"name":"phrases","synonyms":"","value":"Resonance"},{"name":"phrases","synonyms":"","value":"Trigger-level"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME --> JET JET"},{"name":"observables","synonyms":"","value":"P P --> JET JET"}],"last_updated":"2025-09-22T18:12:52","parent_child_join":{"name":"child_datatable","parent":"161624"},"recid":165471,"related_publication":161624,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3965479?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3965480?landing_page=true"}],"title":"Dijet mass distribution (J100)","uuid":"b7df18f0-1b95-4d12-b384-2b9d7458cdbc"},{"abstract":"Observed 95% $\\text{CL}_\\text{S}$ upper limits on the production cross-section times acceptance times branching ratio to jets, $\\sigma \\cdot A \\cdot \\text{BR}$, of  Gaussian-shaped signals of 5%, 10%, and 15% width relative to their peak mass, $m_G$. Also included are the corresponding expected upper limits predicted for the case the $m_{jj}$ distribution is observed to be identical to the background prediction in each bin and the $1\\sigma$  and $2\\sigma$ envelopes of outcomes expected for Poisson fluctuations around the background expectation. Limits are derived from the J50 signal region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J50)/csv","json":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J50)/json","root":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J50)/root","yaml":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J50)/yaml","yoda":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J50)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J50)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"165472","creation_date":"2025-09-01","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG"],"phrases":["Dijet Production","Trigger-level","Dark Matter","Proton-Proton Scattering","Resonance"],"reactions":["P P --> ZPRIME --> JET JET"]},"date":"01 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.161624.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":165472,"inspire_id":"2966134","journal_info":"Phys.Rev.D 112 (2025) 092015","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Dijet Production"},{"name":"phrases","synonyms":"","value":"Resonance"},{"name":"phrases","synonyms":"","value":"Trigger-level"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME --> JET JET"},{"name":"observables","synonyms":"","value":"SIG"}],"last_updated":"2025-09-22T18:12:52","parent_child_join":{"name":"child_datatable","parent":"161624"},"recid":165472,"related_publication":161624,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3965482?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3965483?landing_page=true"}],"title":"Gaussian resonance limits (J50)","uuid":"a3e81954-2593-4b92-bb77-870296f2f64c"},{"abstract":"Observed 95% $\\text{CL}_\\text{S}$ upper limits on the production cross-section times acceptance times branching ratio to jets, $\\sigma \\cdot A \\cdot \\text{BR}$, of  Gaussian-shaped signals of 5%, 10%, and 15% width relative to their peak mass, $m_G$. Also included are the corresponding expected upper limits predicted for the case the $m_{jj}$ distribution is observed to be identical to the background prediction in each bin and the $1\\sigma$  and $2\\sigma$ envelopes of outcomes expected for Poisson fluctuations around the background expectation. Limits are derived from the J100 signal region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J100)/csv","json":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J100)/json","root":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J100)/root","yaml":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J100)/yaml","yoda":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J100)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2966134/Gaussian resonance limits (J100)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"165473","creation_date":"2025-09-01","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["SIG"],"phrases":["Dijet Production","Trigger-level","Dark Matter","Proton-Proton Scattering","Resonance"],"reactions":["P P --> ZPRIME --> JET JET"]},"date":"01 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.161624.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":165473,"inspire_id":"2966134","journal_info":"Phys.Rev.D 112 (2025) 092015","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Dijet Production"},{"name":"phrases","synonyms":"","value":"Resonance"},{"name":"phrases","synonyms":"","value":"Trigger-level"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME --> JET JET"},{"name":"observables","synonyms":"","value":"SIG"}],"last_updated":"2025-09-22T18:12:52","parent_child_join":{"name":"child_datatable","parent":"161624"},"recid":165473,"related_publication":161624,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3965485?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3965486?landing_page=true"}],"title":"Gaussian resonance limits (J100)","uuid":"ed05f615-722d-49a5-987b-d4341a37cb2b"},{"abstract":"Observed 95% $\\text{CL}_\\text{S}$ upper limits on the the value of the coupling to quarks, $g_q$, of the $Z^\\prime$ model as a function of the resonance mass $m_{Z^\\prime}$. Also included are the corresponding expected upper limits predicted for the case the $m_{jj}$ distribution is observed to be identical to the background prediction in each bin and the $1\\sigma$  and $2\\sigma$ envelopes of outcomes expected for Poisson fluctuations around the background expectation. Limits are derived from the J50 signal region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2966134/Z' limits (J50)/csv","json":"https://www.hepdata.net/download/table/ins2966134/Z' limits (J50)/json","root":"https://www.hepdata.net/download/table/ins2966134/Z' limits (J50)/root","yaml":"https://www.hepdata.net/download/table/ins2966134/Z' limits (J50)/yaml","yoda":"https://www.hepdata.net/download/table/ins2966134/Z' limits (J50)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2966134/Z' limits (J50)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"165474","creation_date":"2025-09-01","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["GA"],"phrases":["Dijet Production","Trigger-level","Dark Matter","Proton-Proton Scattering","Resonance"],"reactions":["P P --> ZPRIME --> JET JET"]},"date":"01 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.161624.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":165474,"inspire_id":"2966134","journal_info":"Phys.Rev.D 112 (2025) 092015","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Dijet Production"},{"name":"phrases","synonyms":"","value":"Resonance"},{"name":"phrases","synonyms":"","value":"Trigger-level"},{"name":"phrases","synonyms":"","value":"Dark Matter"},{"name":"reactions","synonyms":"","value":"P P --> ZPRIME --> JET JET"},{"name":"observables","synonyms":"","value":"GA"}],"last_updated":"2025-09-22T18:12:52","parent_child_join":{"name":"child_datatable","parent":"161624"},"recid":165474,"related_publication":161624,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3965488?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3965489?landing_page=true"}],"title":"Z' limits (J50)","uuid":"59be8beb-3d7a-4abc-acb0-8cf6ca20bfb9"},{"abstract":"Observed 95% $\\text{CL}_\\text{S}$ upper limits on the the value of the coupling to quarks, $g_q$, of the $Z^\\prime$ model as a function of the resonance mass $m_{Z^\\prime}$. Also included are the corresponding expected upper limits predicted for the case the $m_{jj}$ distribution is observed to be identical to the background prediction in each bin and the $1\\sigma$  and $2\\sigma$ envelopes of outcomes expected for Poisson fluctuations around the background expectation. 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The search is performed solely on jets reconstructed within the ATLAS trigger to overcome bandwidth limitations imposed on conventional single-jet triggers, which would otherwise reject data from decays of TeV dijet resonances. Collision events with two jets satisfying transverse momentum thresholds of $p_{\\textrm{T}} \\ge 85$ GeV and jet rapidity separation of $|y^{*}|<0.6$ are analysed for dijet resonances with invariant masses from $375$ to $1800$ GeV. A data-driven background estimate is used to model the dijet mass distribution from multijet processes. No significant excess above the expected background is observed. Upper limits are set at $95\\%$ confidence level on coupling values for a benchmark leptophobic axial-vector $Z^{\\prime}$ model and on the production cross-section for a new resonance contributing a Gaussian-distributed line-shape to the dijet mass distribution.","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"observables":["P P --> JET JET","GA","SIG","ACC","N"],"phrases":["Dijet Production","Trigger-level","Dark Matter","Proton-Proton Scattering","Resonance"],"reactions":["P P --> JET JET","P P --> ZPRIME --> JET JET"]},"date":"01 Sep 2025","doc_type":"publication","doi":"10.1103/15p2-bkg8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.161624","id":161624,"inspire_id":"2966134","journal_info":"Phys.Rev.D 112 (2025) 092015","keywords":[],"last_updated":"2025-09-22T18:12:54","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-01-08T00:00:00","recid":161624,"resources":[{"description":"Created with hepdata_lib 0.18.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"Webpage with all figures and tables","type":"html","url":"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2018-39/"},{"description":"arXiv","type":"html","url":"http://arxiv.org/abs/arXiv:2509.01219"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"New York U., Abu Dhabi","full_name":"Abdelhameed, Sara"},{"affiliation":"Gottingen U., II. 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In this paper, leptonic decays of W bosons from 140 fb$^{-1}$ of 13 TeV proton-proton collisions at the LHC, reconstructed in the ATLAS experiment, are used to search for heavy neutral leptons produced through their mixing with muon or electron neutrinos in a scenario with lepton number violation. The search is conducted using prompt leptonic decay signatures. The considered final states require two same-charge leptons or three leptons, while vetoing three-lepton same-flavour topologies. No significant excess over the expected Standard Model backgrounds is found, leading to constraints on the heavy neutral lepton's mixing with muon and electron neutrinos for heavy-neutral-lepton masses. The analysis excludes $|U_{e}|^2$ values above $8\\times 10^{-5}$ and $|U_\u03bc|^2$ values above $5.0 \\times 10^{-5}$ in the full mass range of 8-65 GeV. The strongest constraints are placed on heavy-neutral-lepton masses in the range 15--30 GeV of $|U_{e}|^2 < 1.1 \\times 10^{-5}$ and $|U_\u03bc|^2 < 5 \\times 10^{-6}$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2964565/1/csv","json":"https://www.hepdata.net/download/submission/ins2964565/1/json","root":"https://www.hepdata.net/download/submission/ins2964565/1/root","yaml":"https://www.hepdata.net/download/submission/ins2964565/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2964565/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2964565/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2508.20929","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abdelhameed, Sara","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboelela, Mohammed","Aboulhorma, Asmaa","Abramowicz, Halina"],"collaborations":["ATLAS"],"control_number":"167367","creation_date":"2025-08-28","data":[{"abstract":"Comparison between the data and estimated background at preselection level. 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In this paper, leptonic decays of $W$ bosons from 140 fb$^{-1}$ of 13 TeV proton-proton collisions at the LHC, reconstructed in the ATLAS experiment, are used to search for heavy neutral leptons produced through their mixing with muon or electron neutrinos in a scenario with lepton number violation. The search is conducted using prompt leptonic decay signatures. The considered final states require two same-charge leptons or three leptons, while vetoing three-lepton same-flavour topologies. No significant excess over the expected Standard Model backgrounds is found, leading to constraints on the heavy neutral lepton's mixing with muon and electron neutrinos for heavy-neutral-lepton masses. The analysis excludes $|U_{e}|^2$ values above $8\\times 10^{-5}$ and $|U_{\\mu}|^2$ values above $5.0 \\times 10^{-5}$ in the full mass range of 8-65 GeV. The strongest constraints are placed on heavy-neutral-lepton masses in the range 15-30 GeV of $|U_{e}|^2 < 1.1 \\times 10^{-5}$ and $|U_{\\mu}|^2 < 5 \\times 10^{-6}$.","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Heavy Neutral Leptons","HNLs"]},"date":"28 Aug 2025","doc_type":"publication","doi":"10.1140/epjc/s10052-025-15191-w","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.167367","id":167367,"inspire_id":"2964565","journal_info":"Eur.Phys.J.C 86 (2026) 153","keywords":[],"last_updated":"2025-12-30T16:17:07","parent_child_join":{"name":"parent_publication"},"publication_date":"2026-02-25T00:00:00","recid":167367,"resources":[{"description":"Created with hepdata_lib 0.20.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"Webpage with all figures and tables","type":"html","url":"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2019-35/"},{"description":"arXiv","type":"html","url":"https://arxiv.org/abs/2508.20929"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"New York U., Abu Dhabi","full_name":"Abdelhameed, Sara"},{"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":"Southern Methodist U.","full_name":"Aboelela, Mohammed"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"}],"title":"Search for heavy neutral leptons in decays of W bosons produced in 13 TeV $pp$ collisions using prompt signatures in the ATLAS detector","total_tables":15,"type":["article"],"uuid":"d041f3d6-e06b-48e2-9fe3-85f0f222058a","version":1,"year":"2026"},{"abstract":"A model-agnostic search for Beyond the Standard Model physics is presented, targeting final states with at least four light leptons (electrons or muons). The search regions are separated by event topology and unsupervised machine learning is used to identify anomalous events in the full 140 fb$^{-1}$ of proton-proton collision data collected with the ATLAS detector during Run 2. No significant excess above the Standard Model background expectation is observed. Model-agnostic limits are presented in each topology, along with limits on several benchmark models including vector-like leptons, wino-like charginos and neutralinos, or smuons. Limits are set on the flavourful vector-like lepton model for the first time.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2964453/1/csv","json":"https://www.hepdata.net/download/submission/ins2964453/1/json","root":"https://www.hepdata.net/download/submission/ins2964453/1/root","yaml":"https://www.hepdata.net/download/submission/ins2964453/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2964453/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2964453/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2508.19778","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abdelhameed, Sara","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboelela, Mohammed","Aboulhorma, Asmaa","Abramowicz, Halina"],"collaborations":["ATLAS"],"control_number":"167089","creation_date":"2025-08-27","data":[{"abstract":"Comparison between data and the background prediction for the (a) m<sub>T</sub>(4&#8467;, E<sub>T</sub><sup>miss</sup>), (b) m<sup>high</sup>(3&#8467;), (c) m(Z), (d) E<sub>T</sub><sup>miss</sup>, (e) p<sub>T</sub>(Z), and (f) N<sub>jets</sub> distribution in the (a, d) 2Z 0b, (b, e) 1Z 1b 2SFOS, and (c, f) 0Z 2SFOS region, after requiring the anomaly score to be below the 90&percnt; background rejection point. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The &apos;tt+X&apos; background component includes the tt&#772;Z, and tt&#772;H processes. The &apos;HF &#8467;&apos; (&apos;LF &#8467;&apos;) background component refers to processes containing one non-prompt light lepton from heavy-flavour (light-flavour) hadron decays. The ratio of the data to the background prediction (&apos;Bkg.&apos;) is shown in the lower panel.\n\nThe &apos;Other&apos; contribution is dominated by the tWZ production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure. 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The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 4b/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 4b/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 4b/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 4b/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 4b/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 4b/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167369","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167369,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167369,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078898?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078899?landing_page=true"}],"title":"Figure 4b","uuid":"c7eec895-785b-4225-aa1c-19ade313b0bf"},{"abstract":"Comparison between data and the background prediction for the (a) m<sub>T</sub>(4&#8467;, E<sub>T</sub><sup>miss</sup>), (b) m<sup>high</sup>(3&#8467;), (c) m(Z), (d) E<sub>T</sub><sup>miss</sup>, (e) p<sub>T</sub>(Z), and (f) N<sub>jets</sub> distribution in the (a, d) 2Z 0b, (b, e) 1Z 1b 2SFOS, and (c, f) 0Z 2SFOS region, after requiring the anomaly score to be below the 90&percnt; background rejection point. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The &apos;tt+X&apos; background component includes the tt&#772;Z, and tt&#772;H processes. The &apos;HF &#8467;&apos; (&apos;LF &#8467;&apos;) background component refers to processes containing one non-prompt light lepton from heavy-flavour (light-flavour) hadron decays. The ratio of the data to the background prediction (&apos;Bkg.&apos;) is shown in the lower panel.\n\nThe &apos;Other&apos; contribution is dominated by the tWZ production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure. The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 4c/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 4c/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 4c/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 4c/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 4c/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 4c/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167370","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167370,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167370,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078901?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078902?landing_page=true"}],"title":"Figure 4c","uuid":"9bdc7701-1eca-481a-a29a-8bab6aee1696"},{"abstract":"Comparison between data and the background prediction for the (a) m<sub>T</sub>(4&#8467;, E<sub>T</sub><sup>miss</sup>), (b) m<sup>high</sup>(3&#8467;), (c) m(Z), (d) E<sub>T</sub><sup>miss</sup>, (e) p<sub>T</sub>(Z), and (f) N<sub>jets</sub> distribution in the (a, d) 2Z 0b, (b, e) 1Z 1b 2SFOS, and (c, f) 0Z 2SFOS region, after requiring the anomaly score to be below the 90&percnt; background rejection point. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The &apos;tt+X&apos; background component includes the tt&#772;Z, and tt&#772;H processes. The &apos;HF &#8467;&apos; (&apos;LF &#8467;&apos;) background component refers to processes containing one non-prompt light lepton from heavy-flavour (light-flavour) hadron decays. The ratio of the data to the background prediction (&apos;Bkg.&apos;) is shown in the lower panel.\n\nThe &apos;Other&apos; contribution is dominated by the tWZ production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure. The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 4d/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 4d/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 4d/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 4d/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 4d/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 4d/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167371","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167371,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167371,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078904?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078905?landing_page=true"}],"title":"Figure 4d","uuid":"afbdbecb-11a3-4731-902e-ffe2e3e897ee"},{"abstract":"Comparison between data and the background prediction for the (a) m<sub>T</sub>(4&#8467;, E<sub>T</sub><sup>miss</sup>), (b) m<sup>high</sup>(3&#8467;), (c) m(Z), (d) E<sub>T</sub><sup>miss</sup>, (e) p<sub>T</sub>(Z), and (f) N<sub>jets</sub> distribution in the (a, d) 2Z 0b, (b, e) 1Z 1b 2SFOS, and (c, f) 0Z 2SFOS region, after requiring the anomaly score to be below the 90&percnt; background rejection point. 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The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 4e/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 4e/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 4e/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 4e/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 4e/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 4e/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167372","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167372,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167372,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078907?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078908?landing_page=true"}],"title":"Figure 4e","uuid":"c67c431b-fa0d-4a28-9639-6b6b2faf45a6"},{"abstract":"Comparison between data and the background prediction for the (a) m<sub>T</sub>(4&#8467;, E<sub>T</sub><sup>miss</sup>), (b) m<sup>high</sup>(3&#8467;), (c) m(Z), (d) E<sub>T</sub><sup>miss</sup>, (e) p<sub>T</sub>(Z), and (f) N<sub>jets</sub> distribution in the (a, d) 2Z 0b, (b, e) 1Z 1b 2SFOS, and (c, f) 0Z 2SFOS region, after requiring the anomaly score to be below the 90&percnt; background rejection point. 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The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 4f/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 4f/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 4f/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 4f/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 4f/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 4f/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167373","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167373,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167373,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078910?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078911?landing_page=true"}],"title":"Figure 4f","uuid":"c42441b0-8935-42fd-8e0e-ffedc59a37f9"},{"abstract":"Comparison between data and the background prediction for the (a) N<sub>jets</sub>, (b) E<sub>T</sub><sup>miss</sup>, (c) m(3&#8467;), and (d) H<sub>T</sub><sup>lep</sup> distribution in the (a) HFe CR, (b) HF&mu; CR, (c) LFe CR, and (d) the W&gamma;<sup>*</sup>/tt&#772;&gamma;<sup>*</sup> validation region. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The ratio of the data to the background prediction (&apos;Bkg.&apos;) is shown in the lower panel. The &apos;tt+X&apos; background component includes the tt&#772;W, tt&#772;Z, and tt&#772;H processes. The &apos;Other&apos; contribution in the 2&#8467;SS regions is dominated by the tt&#772; and tt&#772;W production, and in the 3&#8467; regions is dominated by the ZZ + LF production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure. The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5a/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5a/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5a/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5a/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167374","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167374,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167374,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078913?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078914?landing_page=true"}],"title":"Figure 5a","uuid":"4ddfe665-0d16-48f2-b5b4-cb9887f9eaf0"},{"abstract":"Comparison between data and the background prediction for the (a) N<sub>jets</sub>, (b) E<sub>T</sub><sup>miss</sup>, (c) m(3&#8467;), and (d) H<sub>T</sub><sup>lep</sup> distribution in the (a) HFe CR, (b) HF&mu; CR, (c) LFe CR, and (d) the W&gamma;<sup>*</sup>/tt&#772;&gamma;<sup>*</sup> validation region. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The ratio of the data to the background prediction (&apos;Bkg.&apos;) is shown in the lower panel. The &apos;tt+X&apos; background component includes the tt&#772;W, tt&#772;Z, and tt&#772;H processes. The &apos;Other&apos; contribution in the 2&#8467;SS regions is dominated by the tt&#772; and tt&#772;W production, and in the 3&#8467; regions is dominated by the ZZ + LF production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure. The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5b/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5b/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5b/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5b/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5b/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5b/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167375","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167375,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167375,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078916?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078917?landing_page=true"}],"title":"Figure 5b","uuid":"c2e5f4c6-1c92-4fed-bf53-96ab65dfa973"},{"abstract":"Comparison between data and the background prediction for the (a) N<sub>jets</sub>, (b) E<sub>T</sub><sup>miss</sup>, (c) m(3&#8467;), and (d) H<sub>T</sub><sup>lep</sup> distribution in the (a) HFe CR, (b) HF&mu; CR, (c) LFe CR, and (d) the W&gamma;<sup>*</sup>/tt&#772;&gamma;<sup>*</sup> validation region. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The ratio of the data to the background prediction (&apos;Bkg.&apos;) is shown in the lower panel. The &apos;tt+X&apos; background component includes the tt&#772;W, tt&#772;Z, and tt&#772;H processes. The &apos;Other&apos; contribution in the 2&#8467;SS regions is dominated by the tt&#772; and tt&#772;W production, and in the 3&#8467; regions is dominated by the ZZ + LF production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure. The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5c/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5c/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5c/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5c/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5c/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5c/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167376","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167376,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167376,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078919?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078920?landing_page=true"}],"title":"Figure 5c","uuid":"c6eaee5b-8646-4dcd-9f0e-e1a45c71d988"},{"abstract":"Comparison between data and the background prediction for the (a) N<sub>jets</sub>, (b) E<sub>T</sub><sup>miss</sup>, (c) m(3&#8467;), and (d) H<sub>T</sub><sup>lep</sup> distribution in the (a) HFe CR, (b) HF&mu; CR, (c) LFe CR, and (d) the W&gamma;<sup>*</sup>/tt&#772;&gamma;<sup>*</sup> validation region. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The ratio of the data to the background prediction (&apos;Bkg.&apos;) is shown in the lower panel. The &apos;tt+X&apos; background component includes the tt&#772;W, tt&#772;Z, and tt&#772;H processes. The &apos;Other&apos; contribution in the 2&#8467;SS regions is dominated by the tt&#772; and tt&#772;W production, and in the 3&#8467; regions is dominated by the ZZ + LF production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure. The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5d/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5d/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5d/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5d/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5d/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5d/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167377","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167377,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167377,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078922?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078923?landing_page=true"}],"title":"Figure 5d","uuid":"06e9006f-b93e-4f25-825a-aaf386e6c666"},{"abstract":"Comparison between data and the background prediction for the discovery regions included in the model-independent fit, after a background-only fit to data in the five cut-based control regions and ten low-anomaly score discovery regions (&apos;post-fit&apos;). All signal bins are shown (&apos;SR&apos;) together with the low-anomaly score discovery regions (&apos;CR&apos;). The various requirements on the anomaly score corresponding to the specified background rejection cuts (99.9/99/90/50&percnt;) are shown for all the applicable SRs and CRs. The lower panels show the ratio of data to the background estimate (&apos;Bkg&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 6/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 6/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 6/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 6/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 6/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 6/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167378","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167378,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167378,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078925?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078926?landing_page=true"}],"title":"Figure 6","uuid":"3e6b76d9-f674-4768-912e-937161777e74"},{"abstract":"Observed and expected excluded visible cross section limits, &sigma;<sub>vis</sub> for the model-independent regions.\n\nThe various requirements on the anomaly score corresponding to the specified background rejection cuts (99.9/99/90/50&percnt;) are shown for all the applicable regions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 7/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 7/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 7/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 7/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 7/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 7/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167379","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167379,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167379,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078928?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078929?landing_page=true"}],"title":"Figure 7","uuid":"549c0a1e-1048-452a-bdf5-e7a467a0bcbe"},{"abstract":"Comparison between data and the background estimate for the anomaly score distribution used in different benchmark regions, after a background-only fit to data (&apos;post-fit&apos;): (a) 4&#8467; Q=0 0Z 0b 2SFOS e&gt;&mu;, (b) 4&#8467; Q=0 0Z &ge;1b 2SFOS e&gt;&mu;, (c) 4&#8467; Q=0 1Z 0b 2SFOS &mu;&gt;e, (d) 4&#8467; Q=&plusmn;2 0b e&gt;&mu;, (e) 4&#8467; Q=&plusmn;2 &ge;1b &mu;&gt;e, and (f) the three &ge;5&#8467; regions: 0Z 0b &mu;&gt;e, 0Z 0b e&ge;&mu;, and 0Z &ge;1b, defined without AD.\n\nDistributions for one flavourful VLL<sub>e</sub> signal point for a VLL mass of 1 TeV and scalar of 550 GeV, a wino-like chargino and neutralino signal point of mass 1.3 TeV, and a smuon signal point of mass 350 GeV and neutralino mass of 250 GeV are overlaid for comparison. The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. The upward-pointing blue arrow indicates a point for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 9a/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 9a/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 9a/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 9a/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 9a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 9a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167380","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167380,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167380,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078931?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078932?landing_page=true"}],"title":"Figure 9a","uuid":"3bd459e3-615a-46d5-8b92-e07fecd7defb"},{"abstract":"Comparison between data and the background estimate for the anomaly score distribution used in different benchmark regions, after a background-only fit to data (&apos;post-fit&apos;): (a) 4&#8467; Q=0 0Z 0b 2SFOS e&gt;&mu;, (b) 4&#8467; Q=0 0Z &ge;1b 2SFOS e&gt;&mu;, (c) 4&#8467; Q=0 1Z 0b 2SFOS &mu;&gt;e, (d) 4&#8467; Q=&plusmn;2 0b e&gt;&mu;, (e) 4&#8467; Q=&plusmn;2 &ge;1b &mu;&gt;e, and (f) the three &ge;5&#8467; regions: 0Z 0b &mu;&gt;e, 0Z 0b e&ge;&mu;, and 0Z &ge;1b, defined without AD.\n\nDistributions for one flavourful VLL<sub>e</sub> signal point for a VLL mass of 1 TeV and scalar of 550 GeV, a wino-like chargino and neutralino signal point of mass 1.3 TeV, and a smuon signal point of mass 350 GeV and neutralino mass of 250 GeV are overlaid for comparison. The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. 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The expected limits from the dedicated ATLAS search [<a href=\" https://doi.org/10.1007/JHEP05%282025%29075\">JHEP05(2025)075</a>], considering only the 4&#8467; channel, are overlaid in dashed grey lines in (a-d). 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The expected limits from the dedicated ATLAS searches [<a href=\" https://doi.org/10.1007/JHEP07%282021%29167\">JHEP07(2021)167</a>, <a href=\" https://doi.org/10.1007/JHEP12%282023%29081\">JHEP12(2023)081</a>] are overlaid in dashed grey lines. 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The expected limits from the dedicated ATLAS searches [<a href=\" https://doi.org/10.1007/JHEP07%282021%29167\">JHEP07(2021)167</a>, <a href=\" https://doi.org/10.1007/JHEP12%282023%29081\">JHEP12(2023)081</a>] are overlaid in dashed grey lines. The inner and outer bands around the expected limit are the &plusmn;1 &sigma; and &plusmn;2 &sigma; variations including all uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (1 sigma band)/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (1 sigma band)/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (1 sigma band)/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (1 sigma band)/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (1 sigma band)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (1 sigma band)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167399","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t32","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167399,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167399,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078988?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078989?landing_page=true"}],"title":"Figure 11a (1 sigma band)","uuid":"811b04fe-5484-46df-8644-56553334e54a"},{"abstract":"Combined observed and expected limits at 95&percnt; CL for the (a) wino-like chargino and neutralino, and (b) smuon models, as a function of the masses of &chi;&#771;<sup>&plusmn;</sup><sub>1</sub> / &chi;&#771;<sup>0</sup><sub>2</sub> and &chi;&#771;<sup>0</sup><sub>1</sub>, and &mu;<sub>L,R</sub> and &Delta;m (&mu;<sub>L,R</sub>, &chi;&#771;<sup>0</sup><sub>1</sub>), respectively. The expected limits from the dedicated ATLAS searches [<a href=\" https://doi.org/10.1007/JHEP07%282021%29167\">JHEP07(2021)167</a>, <a href=\" https://doi.org/10.1007/JHEP12%282023%29081\">JHEP12(2023)081</a>] are overlaid in dashed grey lines. The inner and outer bands around the expected limit are the &plusmn;1 &sigma; and &plusmn;2 &sigma; variations including all uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (Expected)/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (Expected)/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (Expected)/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (Expected)/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (Expected)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 11a (Expected)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167400","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t33","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167400,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167400,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078991?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078992?landing_page=true"}],"title":"Figure 11a (Expected)","uuid":"b004929b-ceee-4be2-a024-8b655d1a6a13"},{"abstract":"Combined observed and expected limits at 95&percnt; CL for the (a) wino-like chargino and neutralino, and (b) smuon models, as a function of the masses of &chi;&#771;<sup>&plusmn;</sup><sub>1</sub> / &chi;&#771;<sup>0</sup><sub>2</sub> and &chi;&#771;<sup>0</sup><sub>1</sub>, and &mu;<sub>L,R</sub> and &Delta;m (&mu;<sub>L,R</sub>, &chi;&#771;<sup>0</sup><sub>1</sub>), respectively. The expected limits from the dedicated ATLAS searches [<a href=\" https://doi.org/10.1007/JHEP07%282021%29167\">JHEP07(2021)167</a>, <a href=\" https://doi.org/10.1007/JHEP12%282023%29081\">JHEP12(2023)081</a>] are overlaid in dashed grey lines. 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The inner and outer bands around the expected limit are the &plusmn;1 &sigma; and &plusmn;2 &sigma; variations including all uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (2 sigma contour)/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (2 sigma contour)/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (2 sigma contour)/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (2 sigma contour)/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (2 sigma contour)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (2 sigma contour)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167402","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t35","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167402,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167402,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4078997?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4078998?landing_page=true"}],"title":"Figure 11b (2 sigma contour)","uuid":"f2f2e789-7423-4412-b8dc-f7355880a42e"},{"abstract":"Combined observed and expected limits at 95&percnt; CL for the (a) wino-like chargino and neutralino, and (b) smuon models, as a function of the masses of &chi;&#771;<sup>&plusmn;</sup><sub>1</sub> / &chi;&#771;<sup>0</sup><sub>2</sub> and &chi;&#771;<sup>0</sup><sub>1</sub>, and &mu;<sub>L,R</sub> and &Delta;m (&mu;<sub>L,R</sub>, &chi;&#771;<sup>0</sup><sub>1</sub>), respectively. The expected limits from the dedicated ATLAS searches [<a href=\" https://doi.org/10.1007/JHEP07%282021%29167\">JHEP07(2021)167</a>, <a href=\" https://doi.org/10.1007/JHEP12%282023%29081\">JHEP12(2023)081</a>] are overlaid in dashed grey lines. The inner and outer bands around the expected limit are the &plusmn;1 &sigma; and &plusmn;2 &sigma; variations including all uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (1 sigma contour)/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (1 sigma contour)/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (1 sigma contour)/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (1 sigma contour)/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (1 sigma contour)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (1 sigma contour)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167403","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t36","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167403,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167403,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079000?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079001?landing_page=true"}],"title":"Figure 11b (1 sigma contour)","uuid":"d0573cef-b151-4076-9cdb-c13dcda0f68d"},{"abstract":"Combined observed and expected limits at 95&percnt; CL for the (a) wino-like chargino and neutralino, and (b) smuon models, as a function of the masses of &chi;&#771;<sup>&plusmn;</sup><sub>1</sub> / &chi;&#771;<sup>0</sup><sub>2</sub> and &chi;&#771;<sup>0</sup><sub>1</sub>, and &mu;<sub>L,R</sub> and &Delta;m (&mu;<sub>L,R</sub>, &chi;&#771;<sup>0</sup><sub>1</sub>), respectively. The expected limits from the dedicated ATLAS searches [<a href=\" https://doi.org/10.1007/JHEP07%282021%29167\">JHEP07(2021)167</a>, <a href=\" https://doi.org/10.1007/JHEP12%282023%29081\">JHEP12(2023)081</a>] are overlaid in dashed grey lines. The inner and outer bands around the expected limit are the &plusmn;1 &sigma; and &plusmn;2 &sigma; variations including all uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Expected)/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Expected)/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Expected)/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Expected)/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Expected)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Expected)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167404","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t37","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167404,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167404,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079003?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079004?landing_page=true"}],"title":"Figure 11b (Expected)","uuid":"411695c3-95cb-4f25-9e03-37b1da5274c5"},{"abstract":"Combined observed and expected limits at 95&percnt; CL for the (a) wino-like chargino and neutralino, and (b) smuon models, as a function of the masses of &chi;&#771;<sup>&plusmn;</sup><sub>1</sub> / &chi;&#771;<sup>0</sup><sub>2</sub> and &chi;&#771;<sup>0</sup><sub>1</sub>, and &mu;<sub>L,R</sub> and &Delta;m (&mu;<sub>L,R</sub>, &chi;&#771;<sup>0</sup><sub>1</sub>), respectively. The expected limits from the dedicated ATLAS searches [<a href=\" https://doi.org/10.1007/JHEP07%282021%29167\">JHEP07(2021)167</a>, <a href=\" https://doi.org/10.1007/JHEP12%282023%29081\">JHEP12(2023)081</a>] are overlaid in dashed grey lines. The inner and outer bands around the expected limit are the &plusmn;1 &sigma; and &plusmn;2 &sigma; variations including all uncertainties, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Observed)/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Observed)/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Observed)/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Observed)/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Observed)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 11b (Observed)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167405","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t38","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167405,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167405,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079006?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079007?landing_page=true"}],"title":"Figure 11b (Observed)","uuid":"201a4afc-8af0-4f5d-980c-8ebcf35fbab3"},{"abstract":"Comparison between data and the background prediction for the distribution of the b-jet multiplicity in the WZ/ttZ CR after the VV jet multiplicity correction. The background contributions after the likelihood fit to data (&apos;post-fit&apos;) for the background-only hypothesis are shown as filled histograms. The lower panel shows the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;W, tt&#772;Z, and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the tZq production. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The last bin contains the overflow.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 1 from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 1 from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 1 from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 1 from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 1 from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 1 from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167406","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t39","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167406,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167406,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079009?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079010?landing_page=true"}],"title":"Figure 1 from Auxiliary material","uuid":"3efdf123-ea94-494b-b291-14465c8ce207"},{"abstract":"Comparison between data and the background prediction for the event yields in the HF<sub>e</sub> CR, HF<sub>&mu;</sub>, Conversions, and LF<sub>e</sub> CRs, after a background-only fit to data (&apos;Post-fit&apos;). The lower panel shows the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;W, tt&#772;Z, and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the ZZ+LF process. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 2 from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 2 from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 2 from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 2 from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 2 from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 2 from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167407","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t40","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167407,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167407,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079012?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079013?landing_page=true"}],"title":"Figure 2 from Auxiliary material","uuid":"7420bf6b-7bcb-4d8e-94ec-6f4cb7c6d0d5"},{"abstract":"Comparison between data and the background prediction for the discovery regions included in the model-independent fit, before any fit to data (&apos;pre-fit&apos;). All signal bins are shown (&apos;SR&apos;) together with the low-anomaly score discovery regions (&apos;CR&apos;). The various requirements on the anomaly score corresponding to the specified background rejection cuts (99.9/99/90/50&percnt;) are shown for all the applicable SRs and CRs. The lower panels show the ratio of data to the background estimate (&apos;Bkg&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the background prediction is indicated by the blue hatched band. The upward-pointing blue arrows indicate points for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 4 from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 4 from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 4 from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 4 from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 4 from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 4 from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167408","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t41","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167408,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167408,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079015?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079016?landing_page=true"}],"title":"Figure 4 from Auxiliary material","uuid":"b3f81a1d-0cd6-4770-9789-ffe1cefb7487"},{"abstract":"Comparison between data and the background estimate for the anomaly score distribution used in different benchmark regions before any fit to data (&apos;pre-fit&apos;): (a) 4&#8467; Q=0 0Z 0b 2SFOS e&gt;&mu;, (b) 4&#8467; Q=0 0Z &ge;1b 2SFOS e&gt;&mu;, (c) 4&#8467; Q=0 1Z 0b 2SFOS &mu;&gt;e, (d) 4&#8467; Q=&plusmn;2 0b e&gt;&mu;, (e) 4&#8467; Q=&plusmn;2 &ge;1b &mu;&gt;e, and (f) the three &ge;5&#8467; regions: 0Z 0b &mu;&gt;e, 0Z 0b e&ge;&mu;, and 0Z &ge;1b, defined without AD.\n\nDistributions for one flavourful VLL<sub>e</sub> signal point for a VLL mass of 1 TeV and scalar of 550 GeV, a wino-like chargino and neutralino signal point of mass 1.3 TeV, and a smuon signal point of mass 350 GeV and neutralino mass of 250 GeV are overlaid for comparison. The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. The upward-pointing blue arrow indicates a point for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5a from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5a from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5a from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5a from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5a from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5a from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167409","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t42","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167409,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167409,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079018?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079019?landing_page=true"}],"title":"Figure 5a from Auxiliary material","uuid":"9c024fa5-c8a3-404e-9b4c-7d60fa2a8637"},{"abstract":"Comparison between data and the background estimate for the anomaly score distribution used in different benchmark regions before any fit to data (&apos;pre-fit&apos;): (a) 4&#8467; Q=0 0Z 0b 2SFOS e&gt;&mu;, (b) 4&#8467; Q=0 0Z &ge;1b 2SFOS e&gt;&mu;, (c) 4&#8467; Q=0 1Z 0b 2SFOS &mu;&gt;e, (d) 4&#8467; Q=&plusmn;2 0b e&gt;&mu;, (e) 4&#8467; Q=&plusmn;2 &ge;1b &mu;&gt;e, and (f) the three &ge;5&#8467; regions: 0Z 0b &mu;&gt;e, 0Z 0b e&ge;&mu;, and 0Z &ge;1b, defined without AD.\n\nDistributions for one flavourful VLL<sub>e</sub> signal point for a VLL mass of 1 TeV and scalar of 550 GeV, a wino-like chargino and neutralino signal point of mass 1.3 TeV, and a smuon signal point of mass 350 GeV and neutralino mass of 250 GeV are overlaid for comparison. The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. 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The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. The upward-pointing blue arrow indicates a point for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5c from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5c from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5c from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5c from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5c from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5c from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167411","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t44","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167411,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167411,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079024?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079025?landing_page=true"}],"title":"Figure 5c from Auxiliary material","uuid":"159e5eff-205f-4884-ab9f-e422acddc747"},{"abstract":"Comparison between data and the background estimate for the anomaly score distribution used in different benchmark regions before any fit to data (&apos;pre-fit&apos;): (a) 4&#8467; Q=0 0Z 0b 2SFOS e&gt;&mu;, (b) 4&#8467; Q=0 0Z &ge;1b 2SFOS e&gt;&mu;, (c) 4&#8467; Q=0 1Z 0b 2SFOS &mu;&gt;e, (d) 4&#8467; Q=&plusmn;2 0b e&gt;&mu;, (e) 4&#8467; Q=&plusmn;2 &ge;1b &mu;&gt;e, and (f) the three &ge;5&#8467; regions: 0Z 0b &mu;&gt;e, 0Z 0b e&ge;&mu;, and 0Z &ge;1b, defined without AD.\n\nDistributions for one flavourful VLL<sub>e</sub> signal point for a VLL mass of 1 TeV and scalar of 550 GeV, a wino-like chargino and neutralino signal point of mass 1.3 TeV, and a smuon signal point of mass 350 GeV and neutralino mass of 250 GeV are overlaid for comparison. The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. The upward-pointing blue arrow indicates a point for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5d from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5d from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5d from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5d from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5d from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5d from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167412","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t45","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167412,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167412,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079027?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079028?landing_page=true"}],"title":"Figure 5d from Auxiliary material","uuid":"484f7038-54c7-4a39-8bb1-e02e99a7a8f1"},{"abstract":"Comparison between data and the background estimate for the anomaly score distribution used in different benchmark regions before any fit to data (&apos;pre-fit&apos;): (a) 4&#8467; Q=0 0Z 0b 2SFOS e&gt;&mu;, (b) 4&#8467; Q=0 0Z &ge;1b 2SFOS e&gt;&mu;, (c) 4&#8467; Q=0 1Z 0b 2SFOS &mu;&gt;e, (d) 4&#8467; Q=&plusmn;2 0b e&gt;&mu;, (e) 4&#8467; Q=&plusmn;2 &ge;1b &mu;&gt;e, and (f) the three &ge;5&#8467; regions: 0Z 0b &mu;&gt;e, 0Z 0b e&ge;&mu;, and 0Z &ge;1b, defined without AD.\n\nDistributions for one flavourful VLL<sub>e</sub> signal point for a VLL mass of 1 TeV and scalar of 550 GeV, a wino-like chargino and neutralino signal point of mass 1.3 TeV, and a smuon signal point of mass 350 GeV and neutralino mass of 250 GeV are overlaid for comparison. The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. The upward-pointing blue arrow indicates a point for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5e from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5e from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5e from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5e from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5e from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5e from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167413","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t46","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167413,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167413,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079030?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079031?landing_page=true"}],"title":"Figure 5e from Auxiliary material","uuid":"614d2aa1-9ca0-4118-831b-73792d00bf73"},{"abstract":"Comparison between data and the background estimate for the anomaly score distribution used in different benchmark regions before any fit to data (&apos;pre-fit&apos;): (a) 4&#8467; Q=0 0Z 0b 2SFOS e&gt;&mu;, (b) 4&#8467; Q=0 0Z &ge;1b 2SFOS e&gt;&mu;, (c) 4&#8467; Q=0 1Z 0b 2SFOS &mu;&gt;e, (d) 4&#8467; Q=&plusmn;2 0b e&gt;&mu;, (e) 4&#8467; Q=&plusmn;2 &ge;1b &mu;&gt;e, and (f) the three &ge;5&#8467; regions: 0Z 0b &mu;&gt;e, 0Z 0b e&ge;&mu;, and 0Z &ge;1b, defined without AD.\n\nDistributions for one flavourful VLL<sub>e</sub> signal point for a VLL mass of 1 TeV and scalar of 550 GeV, a wino-like chargino and neutralino signal point of mass 1.3 TeV, and a smuon signal point of mass 350 GeV and neutralino mass of 250 GeV are overlaid for comparison. The lower panels show the ratio of data to the background estimate (&apos;Bkg.&apos;). The &apos;tt+X&apos; background component includes the tt&#772;Z (4&#8467; only) and tt&#772;H processes. The &apos;Other&apos; contribution is dominated by the VH process. The size of the combined statistical and systematic uncertainty in the signal-plus-background prediction is indicated by the blue hatched band. The upward-pointing blue arrow indicates a point for which the data-to-background (&apos;Data/Bkg.\u2019) ratio exceeds the vertical range of the figure.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2964453/Figure 5f from Auxiliary material/csv","json":"https://www.hepdata.net/download/table/ins2964453/Figure 5f from Auxiliary material/json","root":"https://www.hepdata.net/download/table/ins2964453/Figure 5f from Auxiliary material/root","yaml":"https://www.hepdata.net/download/table/ins2964453/Figure 5f from Auxiliary material/yaml","yoda":"https://www.hepdata.net/download/table/ins2964453/Figure 5f from Auxiliary material/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2964453/Figure 5f from Auxiliary material/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167414","creation_date":"2025-08-27","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"datatable","doi":"10.17182/hepdata.167089.v1/t47","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167414,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"phrases","synonyms":"","value":"Vectorlike leptons"},{"name":"phrases","synonyms":"","value":"VLL"},{"name":"phrases","synonyms":"","value":"Anomaly detection"},{"name":"phrases","synonyms":"","value":"AD"},{"name":"phrases","synonyms":"","value":"Wino"},{"name":"reactions","synonyms":"","value":"pp -> VLL VLL"}],"last_updated":"2025-12-11T17:24:56","parent_child_join":{"name":"child_datatable","parent":"167089"},"recid":167414,"related_publication":167089,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4079033?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4079034?landing_page=true"}],"title":"Figure 5f from Auxiliary material","uuid":"a25b1efc-7a79-4973-913a-95fe960a6c1e"}],"data_abstract":"A model-agnostic search for Beyond the Standard Model physics is presented, targeting final states with at least four light leptons (electrons or muons). The search regions are separated by event topology and unsupervised machine learning is used to identify anomalous events in the full 140 fb$^{-1}$ of proton-proton collision data collected with the ATLAS detector during Run 2. No significant excess above the Standard Model background expectation is observed. Model-agnostic limits are presented in each topology, along with limits on several benchmark models including vector-like leptons, wino-like charginos and neutralinos, or smuons. Limits are set on the flavourful vector-like lepton model for the first time.","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Vectorlike leptons","Anomaly detection","AD","Wino","VLL"],"reactions":["pp -> VLL VLL"]},"date":"27 Aug 2025","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.167089","id":167089,"inspire_id":"2964453","journal_info":"CERN-EP-2025-189","keywords":[],"last_updated":"2025-12-11T17:25:03","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-12-11T00:00:00","recid":167089,"resources":[{"description":"Created with hepdata_lib 0.20.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"Webpage with all figures and tables","type":"html","url":"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2021-34/"},{"description":"arXiv","type":"html","url":"https://arxiv.org/abs/2508.19778"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"New York U., Abu Dhabi","full_name":"Abdelhameed, Sara"},{"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":"Southern Methodist U.","full_name":"Aboelela, Mohammed"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"}],"title":"Search for Beyond the Standard Model physics with anomaly detection in multilepton final states in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","total_tables":47,"type":["article"],"uuid":"7e295952-69ad-4f1c-97d0-28e9aef06cc6","version":1,"year":"2025"},{"abstract":"A search for Higgs boson pair production in the $b \\overline{b} \u03b3\u03b3$ final state is performed. The proton-proton collision dataset in this analysis corresponds to an integrated luminosity of 308 fb$^{-1}$, consisting of two samples, 140 fb$^{-1}$ at a centre-of-mass energy of 13 TeV and 168 fb$^{-1}$ at 13.6 TeV, recorded between 2015 and 2024 by the ATLAS detector at the CERN Large Hadron Collider. In addition to a larger dataset, this analysis improves upon the previous search in the same final state through several methodological and technical developments. The Higgs boson pair production cross section divided by the Standard Model prediction is found to be $\u03bc_{HH} = 0.9^{+1.4}_{-1.1}$ ($\u03bc_{HH} = 1^{+1.3}_{-1.0}$ expected), which translates into a 95% confidence-level upper limit of $\u03bc_{HH}<3.8$. At the same confidence level the Higgs self-coupling modifier is constrained to be in the range $-1.7 < \u03ba_\u03bb< 6.6$ ($-1.8 < \u03ba_\u03bb< 6.9$ expected).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2943676/1/csv","json":"https://www.hepdata.net/download/submission/ins2943676/1/json","root":"https://www.hepdata.net/download/submission/ins2943676/1/root","yaml":"https://www.hepdata.net/download/submission/ins2943676/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2943676/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2943676/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2507.03495","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abdelhameed, Sara","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboelela, Mohammed","Aboulhorma, Asmaa","Abramowicz, Halina"],"collaborations":["ATLAS"],"control_number":"160696","creation_date":"2025-07-04","data":[{"abstract":"Weighted di-photon invariant mass distribution summed over all categories and the two data-taking periods. 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The scan is performed by floating the indicated parameter of interest while fixing all the others to their SM value.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943676/Table 29 ($%5Ckappa_{%5Clambda}$ exp aux)/csv","json":"https://www.hepdata.net/download/table/ins2943676/Table 29 ($%5Ckappa_{%5Clambda}$ exp aux)/json","root":"https://www.hepdata.net/download/table/ins2943676/Table 29 ($%5Ckappa_{%5Clambda}$ exp aux)/root","yaml":"https://www.hepdata.net/download/table/ins2943676/Table 29 ($%5Ckappa_{%5Clambda}$ exp aux)/yaml","yoda":"https://www.hepdata.net/download/table/ins2943676/Table 29 ($%5Ckappa_{%5Clambda}$ exp aux)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943676/Table 29 ($%5Ckappa_{%5Clambda}$ exp aux)/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"166073","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"observables":["$\\kappa_{\\lambda}$","$-2ln\\Lambda$","Likelihood"],"phrases":["Events","bb","Higgs boson pair","diphoton","Proton-Proton","Higgs boson","gamma gamma"],"reactions":["P P --> HIGGS HIGGS --> BQ BQBAR GAMMA GAMMA"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.160696.v1/t29","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":166073,"inspire_id":"2943676","journal_info":"CERN-EP-2025-140","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGS HIGGS --> BQ BQBAR GAMMA GAMMA"},{"name":"observables","synonyms":"","value":"Likelihood"},{"name":"observables","synonyms":"","value":"$\\kappa_{\\lambda}$"},{"name":"observables","synonyms":"","value":"$-2ln\\Lambda$"},{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"Events"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgs boson"},{"name":"phrases","synonyms":"","value":"Higgs boson pair"},{"name":"phrases","synonyms":"","value":"gamma gamma"},{"name":"phrases","synonyms":"","value":"diphoton"},{"name":"phrases","synonyms":"","value":"bb"}],"last_updated":"2025-10-20T19:14:45","parent_child_join":{"name":"child_datatable","parent":"160696"},"recid":166073,"related_publication":160696,"resources":[{"description":"Image file","type":"pdf","url":"https://www.hepdata.net/record/resource/3993339?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3993340?landing_page=true"}],"title":"Table 29 ($\\kappa_{\\lambda}$ exp aux)","uuid":"ff8dbc06-3280-40c1-a7a4-e9bd34c046a6"},{"abstract":"The expected number of events (estimated by using simulation) from the SM HH signals and single Higgs boson production, and the expected number of events from the continuum background, evaluated in the 120 GeV < $m_{\\gamma\\gamma}$ < 130 GeV window in Run 3 for the different low-mass (LM) and high-mass (HM) categories. For comparison, the number of data events is also shown. The uncertainties in the HH signals and single Higgs boson backgrounds include the systematic uncertainties discussed in Section 6. Asymmetric uncertainties arise primarily from the theory calculation of the SM ggF HH cross section and the large uncertainty in the yield of single Higgs bosons produced in ggF events in association with heavy-flavour jets. The uncertainty in the continuum background is given by the sum in quadrature of the statistical uncertainty from the fit to the data and the spurious signal uncertainty.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943676/Table 30/csv","json":"https://www.hepdata.net/download/table/ins2943676/Table 30/json","root":"https://www.hepdata.net/download/table/ins2943676/Table 30/root","yaml":"https://www.hepdata.net/download/table/ins2943676/Table 30/yaml","yoda":"https://www.hepdata.net/download/table/ins2943676/Table 30/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943676/Table 30/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"166074","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0}],"observables":["expected yields"],"phrases":["Events","bb","Higgs boson pair","diphoton","Proton-Proton","Higgs boson","gamma gamma"],"reactions":["P P --> HIGGS HIGGS --> BQ BQBAR GAMMA GAMMA"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.160696.v1/t30","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":166074,"inspire_id":"2943676","journal_info":"CERN-EP-2025-140","keywords":[{"name":"reactions","synonyms":"","value":"P P --> HIGGS HIGGS --> BQ BQBAR GAMMA GAMMA"},{"name":"observables","synonyms":"","value":"expected yields"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"Events"},{"name":"phrases","synonyms":"","value":"Proton-Proton"},{"name":"phrases","synonyms":"","value":"Higgs boson"},{"name":"phrases","synonyms":"","value":"Higgs boson pair"},{"name":"phrases","synonyms":"","value":"gamma gamma"},{"name":"phrases","synonyms":"","value":"diphoton"},{"name":"phrases","synonyms":"","value":"bb"}],"last_updated":"2025-10-20T19:14:45","parent_child_join":{"name":"child_datatable","parent":"160696"},"recid":166074,"related_publication":160696,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3993342?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3993343?landing_page=true"}],"title":"Table 30","uuid":"b1de08a4-3a2a-4c31-b05e-01f00080a282"}],"data_abstract":"A search for Higgs boson pair production in the $b \\overline{b} \\gamma \\gamma$ final state is performed. The proton-proton collision dataset in this analysis corresponds to an integrated luminosity of 308 fb$^{-1}$, consisting of two samples, with 140 fb$^{-1}$ at a centre-of-mass energy of 13 TeV and 168 fb$^{-1}$ at 13.6 TeV, recorded between 2015 and 2024 by the ATLAS detector at the CERN Large Hadron Collider. Compared to the result of a previous search in the same final state, in addition to the increased dataset, the analysis incorporates several methodological and technical improvements. The Higgs boson pair production cross section divided by the Standard Model prediction is found to be  $\\mu_{HH} = 0.9^{+1.4}_{-1.1}$ ($\\mu_{HH} = 1^{+1.3}_{-1.0}$ expected), which translates into a 95% confidence-level upper limit of $\\mu_{HH}<3.8$. At the same confidence level the Higgs self-coupling modifier is constrained to be in the range $-1.7 < \\kappa_\\lambda < 6.6$  ($-1.8 < \\kappa_\\lambda < 6.9$ expected).\n","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"observables":["$\\kappa_{2V}$","$-2ln\\Lambda$","expected yields","$\\kappa_{\\lambda}$","signal strength","Likelihood","$m_{\\gamma\\gamma}$"],"phrases":["Events","Higgs boson pair","diphoton","bb","Proton-Proton","Higgs boson","gamma gamma"],"reactions":["P P --> HIGGS HIGGS --> BQ BQBAR GAMMA GAMMA"]},"date":"04 Jul 2025","doc_type":"publication","doi":null,"first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.160696","id":160696,"inspire_id":"2943676","journal_info":"CERN-EP-2025-140","keywords":[],"last_updated":"2025-10-20T19:14:49","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-10-20T00:00:00","recid":160696,"resources":[],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},{"affiliation":"Bergen U.","full_name":"Aakvaag, Erlend"},{"affiliation":"Oklahoma U.","full_name":"Abbott, Braden Keim"},{"affiliation":"New York U., Abu Dhabi","full_name":"Abdelhameed, Sara"},{"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":"Southern Methodist U.","full_name":"Aboelela, Mohammed"},{"affiliation":"Mohammed V U., Agdal","full_name":"Aboulhorma, Asmaa"},{"affiliation":"Tel Aviv U.","full_name":"Abramowicz, Halina"}],"title":"Study of Higgs boson pair production in the $HH \\rightarrow b \\overline{b} \\gamma\\gamma$ final state with 308 fb$^{-1}$ of data collected at $\\sqrt{s} = 13$ TeV and 13.6 TeV by the ATLAS experiment","total_tables":30,"type":["article"],"uuid":"d1137dc4-767b-4477-a9d6-e7bc5e7b3549","version":1,"year":"2025"},{"abstract":"This paper presents a search for physics beyond the Standard Model targeting a heavy resonance visible in the invariant mass of the lepton-jet system. The analysis focuses on final states with a high-energy lepton and jet, and is optimised for the resonant production of leptoquarks-a novel production mode mediated by the lepton content of the proton originating from quantum fluctuations. Four distinct and orthogonal final states are considered: $e$+light jet, $\u03bc$+light jet, $e$+$b$-jet, and $\u03bc$+$b$-jet, constituting the first search at the Large Hadron Collider for resonantly produced leptoquarks with couplings to electrons and muons. Events with an additional same-flavour lepton, as expected from higher-order diagrams in the signal process, are also included in each channel. The search uses proton-proton collision data from the full Run 2, corresponding to an integrated luminosity of 140 fb$^{-1}$ at a centre-of-mass energy of $\\sqrt{s} = 13$ TeV, and from a part of Run 3 (2022-2023), corresponding to 55 fb$^{-1}$ at $\\sqrt{s} = 13.6$ TeV. No significant excess over Standard Model predictions is observed. The results are interpreted as exclusion limits on scalar leptoquark ($\\tilde{S}_1$) production, substantially improving upon previous ATLAS constraints from leptoquark pair production for large coupling values. The excluded $\\tilde{S}_1$ mass ranges depend on the coupling strength, reaching up to 3.4 TeV for quark-lepton couplings $y_{de} = 1.0$, and up to 4.3 TeV, 3.1 TeV, and 2.8 TeV for $y_{s\u03bc}$, $y_{be}$, and $y_{b\u03bc}$ couplings set to 3.5, respectively.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2943627/1/csv","json":"https://www.hepdata.net/download/submission/ins2943627/1/json","root":"https://www.hepdata.net/download/submission/ins2943627/1/root","yaml":"https://www.hepdata.net/download/submission/ins2943627/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2943627/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2943627/1/yoda.h5"}},"analyses":[{"analysis":"https://www.hepdata.net/record/resource/4054696?landing_page=true","filename":"likelihoods.tar.gz","type":"HistFactory"}],"arxiv_id":"arXiv:2507.03650","authors":["Aad, Georges","Aakvaag, Erlend","Abbott, Braden Keim","Abdelhameed, Sara","Abeling, Kira","Abicht, Nils Julius","Abidi, Haider","Aboelela, Mohammed","Aboulhorma, Asmaa","Abramowicz, Halina"],"collaborations":["ATLAS"],"control_number":"166328","creation_date":"2025-07-04","data":[{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-ej and (c, d) SR-2L-ej of the e+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (2.0&nbsp;TeV, 1.0) and S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (3.0&nbsp;TeV, 1.0), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 10a/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 10a/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 10a/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 10a/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 10a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 10a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167115","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t1","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167115,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167115,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054698?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054699?landing_page=true"}],"title":"Figure 10a","uuid":"b5bebddf-be61-4552-b00b-73eb96836536"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-ej and (c, d) SR-2L-ej of the e+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (2.0&nbsp;TeV, 1.0) and S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (3.0&nbsp;TeV, 1.0), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 10b/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 10b/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 10b/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 10b/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 10b/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 10b/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167116","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t2","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167116,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167116,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054701?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054702?landing_page=true"}],"title":"Figure 10b","uuid":"500f1b57-b439-4d83-bdf6-582c0029efb9"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-ej and (c, d) SR-2L-ej of the e+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (2.0&nbsp;TeV, 1.0) and S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (3.0&nbsp;TeV, 1.0), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 10c/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 10c/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 10c/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 10c/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 10c/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 10c/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167117","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t3","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167117,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167117,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054704?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054705?landing_page=true"}],"title":"Figure 10c","uuid":"ff972d51-8b8c-4aab-8fbe-68fbf8edba56"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-ej and (c, d) SR-2L-ej of the e+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (2.0&nbsp;TeV, 1.0) and S&#771;<sub>1</sub> (m, y<sub>de</sub>) = (3.0&nbsp;TeV, 1.0), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 10d/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 10d/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 10d/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 10d/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 10d/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 10d/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167118","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t4","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167118,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167118,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054707?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054708?landing_page=true"}],"title":"Figure 10d","uuid":"4f2ac359-0f83-43b2-b509-dfd1506ce8e1"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;j and (c, d) SR-2L-&mu;j of the &mu;+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (2.0&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (3.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 11a/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 11a/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 11a/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 11a/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 11a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 11a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167119","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t5","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167119,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167119,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054710?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054711?landing_page=true"}],"title":"Figure 11a","uuid":"e9383fe4-5634-48cd-87d0-83c57226c48e"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;j and (c, d) SR-2L-&mu;j of the &mu;+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (2.0&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (3.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 11b/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 11b/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 11b/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 11b/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 11b/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 11b/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167120","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t6","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167120,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167120,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054713?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054714?landing_page=true"}],"title":"Figure 11b","uuid":"af10a483-ee85-4a43-ae6e-72ba0519d422"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;j and (c, d) SR-2L-&mu;j of the &mu;+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (2.0&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (3.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 11c/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 11c/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 11c/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 11c/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 11c/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 11c/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167121","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t7","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167121,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167121,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054716?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054717?landing_page=true"}],"title":"Figure 11c","uuid":"b7060144-db55-4e86-904a-d80005bfd3ae"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;j and (c, d) SR-2L-&mu;j of the &mu;+light-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (2.0&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>s&mu;</sub>) = (3.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 11d/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 11d/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 11d/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 11d/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 11d/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 11d/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167122","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t8","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167122,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167122,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054719?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054720?landing_page=true"}],"title":"Figure 11d","uuid":"51099d05-aebf-4b58-ac20-f06462f62f65"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-eb and (c, d) SR-2L-eb of the e+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (1.5&nbsp;TeV, 2.5) and S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (2.0&nbsp;TeV, 2.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 12a/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 12a/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 12a/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 12a/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 12a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 12a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167123","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t9","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167123,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167123,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054722?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054723?landing_page=true"}],"title":"Figure 12a","uuid":"4460cce1-8870-4cc3-b973-30ad7d4beeb7"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-eb and (c, d) SR-2L-eb of the e+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (1.5&nbsp;TeV, 2.5) and S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (2.0&nbsp;TeV, 2.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 12b/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 12b/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 12b/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 12b/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 12b/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 12b/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167124","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t10","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167124,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167124,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054725?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054726?landing_page=true"}],"title":"Figure 12b","uuid":"2fe68152-02bc-4bdc-94cc-5b2bb02a4896"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-eb and (c, d) SR-2L-eb of the e+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (1.5&nbsp;TeV, 2.5) and S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (2.0&nbsp;TeV, 2.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 12c/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 12c/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 12c/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 12c/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 12c/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 12c/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167125","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t11","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167125,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167125,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054728?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054729?landing_page=true"}],"title":"Figure 12c","uuid":"0d51209b-2a6e-4445-83bc-005b5b61cbd2"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-eb and (c, d) SR-2L-eb of the e+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (1.5&nbsp;TeV, 2.5) and S&#771;<sub>1</sub> (m, y<sub>be</sub>) = (2.0&nbsp;TeV, 2.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 12d/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 12d/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 12d/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 12d/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 12d/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 12d/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167126","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t12","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167126,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167126,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054731?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054732?landing_page=true"}],"title":"Figure 12d","uuid":"137ae008-58ad-4bfb-90a0-c4a3fe0546e7"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;b and (c, d) SR-2L-&mu;b of the &mu;+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (1.5&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (2.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 13a/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 13a/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 13a/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 13a/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 13a/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 13a/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167127","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t13","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167127,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167127,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054734?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054735?landing_page=true"}],"title":"Figure 13a","uuid":"df50dc5c-958d-446a-bb94-f07ae5d39d72"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;b and (c, d) SR-2L-&mu;b of the &mu;+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (1.5&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (2.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 13b/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 13b/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 13b/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 13b/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 13b/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 13b/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167128","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t14","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167128,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167128,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054737?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054738?landing_page=true"}],"title":"Figure 13b","uuid":"becace33-cbfd-4f17-8e53-62b586021d58"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;b and (c, d) SR-2L-&mu;b of the &mu;+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (1.5&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (2.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 13c/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 13c/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 13c/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 13c/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 13c/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 13c/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167129","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t15","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167129,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167129,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054740?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054741?landing_page=true"}],"title":"Figure 13c","uuid":"7cbc0e30-4152-4a23-8340-f1f854c992d4"},{"abstract":"Data (dots) and post-fit SM distribution (histograms) of m<sub>&#8467;j</sub> in (a, b) SR-1L-&mu;b and (c, d) SR-2L-&mu;b of the &mu;+b-jet channel obtained by a CR+SR background-only fit for Run&nbsp;2 and Run&nbsp;3, respectively. The lower panel shows the ratio of observed data to the total post- and pre-fit SM prediction. The last bin includes the overflow. Uncertainties in the background estimates include both the statistical and systematic uncertainties, with correlations between uncertainties taken into account. The dashed lines show the predicted yields for two benchmark signal models corresponding to S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (1.5&nbsp;TeV, 1.5) and S&#771;<sub>1</sub> (m, y<sub>b&mu;</sub>) = (2.0&nbsp;TeV, 1.5), respectively.\n\nNote: the values in the table are normalized by the width of corresponding bin","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 13d/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 13d/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 13d/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 13d/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 13d/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 13d/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167130","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t16","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167130,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167130,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054743?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054744?landing_page=true"}],"title":"Figure 13d","uuid":"380a8a6f-b263-4655-9851-191be389a1fd"},{"abstract":"Exclusion limits for minimal models of S&#771;<sub>1</sub> production with only y<sub>de</sub> being non-zero obtained from a simultaneous fit to SR-1L and SR-2L of the e+light-jet channel combining Run-2 and Run-3 data. All limits are computed at 95&percnt; CL and the observed (red solid lines) and expected (black dashed lines) exclusion limits are shown in the m(S&#771;<sub>1</sub>) &ndash; y<sub>de</sub> plane. The observed exclusion should be interpreted as the region above the red line. The yellow inner (green outer) shaded band around the expected limits corresponds to the &plusmn;1 &sigma; (&plusmn;2 &sigma;) variations of the expected limit, accounting for all uncertainties. The observed limit obtained from ATLAS searches for LQ pair production is also shown as dark blue line [13]. Constraints from weak charge measurements of protons and nuclei on y<sub>de</sub> couplings derived by Ref. [10] are shown as light magenta line.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 14/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 14/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 14/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 14/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 14/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 14/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167131","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t17","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167131,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167131,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054746?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054747?landing_page=true"}],"title":"Figure 14","uuid":"11676f11-4a93-4666-a12b-4cdc49a6608e"},{"abstract":"Exclusion limits for minimal models of S&#771;<sub>1</sub> production with only y<sub>s&mu;</sub> being non-zero obtained from a simultaneous fit to SR-1L and SR-2L of the &mu;+light-jet channel combining Run-2 and Run-3 data. All limits are computed at 95&percnt; CL and the observed (red solid lines) and expected (black dashed lines) exclusion limits are shown in the m(S&#771;<sub>1</sub>) &ndash; y<sub>s&mu;</sub> plane. The observed exclusion should be interpreted as the region above the red line. The yellow inner (green outer) shaded band around the expected limits corresponds to the &plusmn;1 &sigma; (&plusmn;2 &sigma;) variations of the expected limit, accounting for all uncertainties. The observed limit obtained from ATLAS searches for LQ pair production is also shown as dark blue line [13].","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 15/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 15/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 15/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 15/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 15/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 15/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167132","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t18","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167132,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167132,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054749?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054750?landing_page=true"}],"title":"Figure 15","uuid":"f4990732-04fb-44ed-bee4-c2ab6bededec"},{"abstract":"Exclusion limits for minimal models of S&#771;<sub>1</sub> production with only y<sub>be</sub> being non-zero obtained from a simultaneous fit to SR-1L and SR-2L of the e+b-jet channel combining Run-2 and Run-3 data. 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The observed limit obtained from ATLAS searches for LQ pair production is also shown as dark blue line [13].","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2943627/Figure 16/csv","json":"https://www.hepdata.net/download/table/ins2943627/Figure 16/json","root":"https://www.hepdata.net/download/table/ins2943627/Figure 16/root","yaml":"https://www.hepdata.net/download/table/ins2943627/Figure 16/yaml","yoda":"https://www.hepdata.net/download/table/ins2943627/Figure 16/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2943627/Figure 16/yoda.h5"}},"authors":null,"collaborations":["ATLAS"],"control_number":"167133","creation_date":"2025-07-04","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"datatable","doi":"10.17182/hepdata.166328.v1/t19","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"id":167133,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"cmenergies","synonyms":"","value":"13600"},{"name":"phrases","synonyms":"","value":"BSM"},{"name":"phrases","synonyms":"","value":"LQ"}],"last_updated":"2025-11-25T18:53:07","parent_child_join":{"name":"child_datatable","parent":"166328"},"recid":167133,"related_publication":166328,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4054752?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4054753?landing_page=true"}],"title":"Figure 16","uuid":"918c13c9-a5d8-45a3-b8ba-0a2eec65dd4c"},{"abstract":"Exclusion limits for minimal models of S&#771;<sub>1</sub> production with only y<sub>b&mu;</sub> being non-zero obtained from a simultaneous fit to SR-1L and SR-2L of the &mu;+b-jet channel combining Run-2 and Run-3 data. 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The excluded $\\tilde{S}_1$ mass ranges depend on the coupling strength, reaching up to 3.4 TeV for quark\u2013lepton couplings $y_{de} = 1.0$, and up to 4.3 TeV, 3.1 TeV, and 2.8 TeV for $y_{s\\mu}$, $y_{be}$, and $y_{b\\mu}$ couplings set to 3.5, respectively.","data_keywords":{"cmenergies":[{"gte":13600.0,"lte":13600.0},{"gte":13000.0,"lte":13000.0}],"phrases":["BSM","LQ"]},"date":"04 Jul 2025","doc_type":"publication","doi":"10.1007/JHEP12(2025)180","first_author":{"affiliation":"Marseille, CPPM","full_name":"Aad, Georges"},"hepdata_doi":"10.17182/hepdata.166328","id":166328,"inspire_id":"2943627","journal_info":"JHEP 12 (2025) 180","keywords":[{"source":"author","value":"Hadron-Hadron Scattering"}],"last_updated":"2025-11-25T18:53:16","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-02-06T00:00:00","recid":166328,"resources":[{"description":"Created with hepdata_lib 0.20.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"Webpage with all figures and tables","type":"html","url":"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2024-12/"},{"description":"arXiv","type":"html","url":"https://arxiv.org/abs/123.11"},{"description":"Tarball containing the full likelihoods in the HistFactory JSON format. 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The data sample, recorded with the ATLAS experiment during Run 2 of the LHC, corresponds to an integrated luminosity of $140~\\text{fb}^{-1}$. Events with one electron and one muon of opposite electric charge in the final state are selected to measure the $t\\bar{t}+1\\text{-jet}$ differential cross-section as a function of the inverse of the invariant mass of the $t\\bar{t}+1\\text{-jet}$ system. Iterative Bayesian Unfolding is used to correct the data to enable comparison with fixed-order calculations at next-to-leading-order accuracy in the strong coupling. The process $pp \\to t\\bar{t}j$ ($2 \\rightarrow 3$), where top quarks are taken as stable particles, and the process $pp \\to b\\bar{b}l^+\u03bdl^- \\bar\u03bd j$ ($2 \\to 7$), which includes top-quark decays to the dilepton final state and off-shell effects, are considered. The top-quark mass is extracted using a $\u03c7^2$ fit of the unfolded normalized differential cross-section distribution. The results obtained with the $2 \\to 3$ and $2 \\to 7$ calculations are compatible within theoretical uncertainties, providing an important consistency check. 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