{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.85748.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1704138"}},{"@id":"https://doi.org/10.1103/PhysRevD.99.052005","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"CERN-LHC. A search for hadronic decays of neutral, weakly interacting, long-lived particles in proton-proton collisions at a centre-of-mass energy of 13 TeV is presented. The data sample used, collected during 2015+2016 ATLAS data-taking period, has a total integrated luminosity of 36.1 fb$^{-1}$. The analysis searches for events with two displaced vertices in the MS, or one displaced vertex in the MS in association with additional activity in the detector that improves the sensitivity for longer lifetimes. Three separate strategies are studied, defined by the number of MS vertices and additional selection criteria. The observed numbers of events are consistent with the expected background and limits for several benchmark signals are determined.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t1","@type":"Dataset","description":"- - - - - - - - - - - - - - - - - - - -...","name":"Overview"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t2","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=100$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t3","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=125$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t4","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=200$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t5","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=400$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t6","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=600$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t7","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=1000$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t8","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for all Stealth SUSY benchmark samples. The trigger efficiency is defined as...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t9","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow \\nu b \\bar{b}$ benchmark samples ($m_{h}=125$ GeV). The...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t10","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow cbs$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t11","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow lcb$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t12","@type":"Dataset","description":"Barrel Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow \\tau\\tau\\nu$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t13","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=100$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t14","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=125$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t15","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=200$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t16","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=400$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t17","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=600$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t18","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for $m_{\\Phi}=1000$ GeV scalar benchmark samples. The trigger efficiency is defined as...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t19","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for all Stealth SUSY benchmark samples. The trigger efficiency is defined as...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t20","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow \\nu b \\bar{b}$ benchmark samples ($m_{h}=125$ GeV). The...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t21","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow cbs$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t22","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow lcb$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t23","@type":"Dataset","description":"Endcap Muon RoI Cluster trigger efficiencies (in %) for baryogenesis $\\chi \\rightarrow \\tau\\tau\\nu$ benchmark samples ($m_{h}=125$ GeV). The trigger efficiency...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t24","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for $m_{\\Phi}=100$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t25","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for $m_{\\Phi}=125$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t26","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for $m_{\\Phi}=200$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t27","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for $m_{\\Phi}=400$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t28","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for $m_{\\Phi}=600$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t29","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for $m_{\\Phi}=1000$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t30","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for all Stealth SUSY benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t31","@type":"Dataset","description":"Barrel MS vertex efficiencies (in %) for baryogenesis $\\chi \\rightarrow \\nu b \\bar{b}$ benchmark samples ($m_{h}=125$ GeV). 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The vertex reconstruction efficiency is...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t35","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for $m_{\\Phi}=100$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t36","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for $m_{\\Phi}=125$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t37","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for $m_{\\Phi}=200$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t38","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for $m_{\\Phi}=400$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t39","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for $m_{\\Phi}=600$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t40","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for $m_{\\Phi}=1000$ GeV scalar benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t41","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for all Stealth SUSY benchmark samples. The vertex reconstruction efficiency is defined as the...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t42","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for baryogenesis $\\chi \\rightarrow \\nu b \\bar{b}$ benchmark samples ($m_{h}=125$ GeV). The vertex reconstruction...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t43","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for baryogenesis $\\chi \\rightarrow cbs$ benchmark samples ($m_{h}=125$ GeV). The vertex reconstruction efficiency is...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.85748.v1/t44","@type":"Dataset","description":"Endcap MS vertex efficiencies (in %) for baryogenesis $\\chi \\rightarrow lcb$ benchmark samples ($m_{h}=125$ GeV). 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