{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.78697.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1630632"}},{"@id":"https://doi.org/10.1103/PhysRevD.97.052012","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"CERN-LHC. A search for long-lived, massive particles predicted by many theories beyond the Standard Model is presented. The search targets final states with large missing transverse momentum and at least one high-mass displaced vertex with five or more tracks, and uses 32.8 fb$^{-1}$ of $\\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the LHC. The observed yield is consistent with the expected background. The results are used to extract 95% CL exclusion limits on the production of long-lived gluinos with masses up to 2.37 TeV and lifetimes of $\\mathcal{O}(10^{-2})\\text{--}\\mathcal{O}(10)$ ns in a simplified model inspired by Split Supersymmetry.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t1","@type":"Dataset","description":"Vertex reconstruction efficiency as a function of radial position $R$ with and without the special LRT processing for one $R$-hadron...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t2","@type":"Dataset","description":"Vertex reconstruction efficiency as a function of radial position $R$ for two $R$-hadron signal samples with $m_{\\tilde{g}} = 1.2$ TeV,...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t3","@type":"Dataset","description":"Fractions of selected events for several signal MC samples with a gluino lifetime $\\tau = 1$ ns, illustrating how $\\mathcal{A}\\times\\varepsilon$...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t4","@type":"Dataset","description":"Fractions of selected events for several signal MC samples with a mass difference $\\Delta m = 100$ GeV, illustrating how...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t5","@type":"Dataset","description":"Two-dimensional distribution of $m_{\\mathrm{DV}}$ and track multiplicity for DVs in data events and events of a $R$-hadron signal sample with...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t6","@type":"Dataset","description":"Two-dimensional distribution of $m_{\\mathrm{DV}}$ and track multiplicity for DVs in data events and events of a $R$-hadron signal sample with...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t7","@type":"Dataset","description":"Upper 95% CL limits on the signal cross section for $m_{\\tilde{g}}=1.4$ TeV and fixed $m_{\\tilde{\\chi}_{1}^{0}}=100$ GeV as a function of...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t8","@type":"Dataset","description":"Upper 95% CL limits on the signal cross section for $m_{\\tilde{g}}=2.0$ TeV and fixed $m_{\\tilde{\\chi}_{1}^{0}}=100$ GeV as a function of...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t9","@type":"Dataset","description":"Lower 95% CL limits on $m_{\\tilde{g}}$ for fixed $m_{\\tilde{\\chi}_{1}^{0}}=100$ GeV as a function of lifetime $\\tau$.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t10","@type":"Dataset","description":"Upper 95% CL limits on the signal cross section for $m_{\\tilde{g}}=1.4$ TeV and fixed $\\Delta m=100$ GeV as a function...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t11","@type":"Dataset","description":"Upper 95% CL limits on the signal cross section for $m_{\\tilde{g}}=2.0$ TeV and fixed $\\Delta m=100$ GeV as a function...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t12","@type":"Dataset","description":"Lower 95% CL limit on $m_{\\tilde{g}}$ for fixed $\\Delta m=100$ GeV as a function of lifetime $\\tau$.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t13","@type":"Dataset","description":"Upper 95% CL limits on the signal cross section for $m_{\\tilde{g}}=1.4$ TeV and fixed $\\tau=1$ ns as a function of...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t14","@type":"Dataset","description":"Upper 95% CL limits on the signal cross section for $m_{\\tilde{g}}=2.0$ TeV and fixed $\\tau=1$ ns as a function of...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t15","@type":"Dataset","description":"Observed 95% CL limit as a function of $m_{\\tilde{g}}$ and $m_{\\tilde{\\chi}_{1}^{0}}$ for fixed $\\tau=1$ ns.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t16","@type":"Dataset","description":"Two-dimensional distributions of $x$-$y$ positions of vertices observed in the data passing the vertex pre-selection and satisfying all signal region...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t17","@type":"Dataset","description":"Distribution of the mass $m_{\\mathrm{DV}}$ for vertices in data events and in events of five $R$-hadron signal samples with $m_{\\tilde{g}}...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t18","@type":"Dataset","description":"Distribution of the track multiplicity $n_{\\mathrm{Tracks}}$ for vertices in data events and events of five $R$-hadron signal samples with $m_{\\tilde{g}}...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t19","@type":"Dataset","description":"Observed cross section upper 95% CL limits as a function of $m_{\\tilde{g}}$ and $\\tau$ for $m_{\\tilde{\\chi}_{1}^{0}}=100$ GeV. For the mass...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t20","@type":"Dataset","description":"Observed cross section upper 95% CL limits as a function of $m_{\\tilde{g}}$ and $\\tau$ for $\\Delta m=100$ GeV. For the...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t21","@type":"Dataset","description":"Observed cross section upper 95% CL limits as a function of $m_{\\tilde{\\chi}_{1}^{0}}$ and $m_{\\tilde{g}}$ for $\\tau = 1$ ns. For...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t22","@type":"Dataset","description":"Parameterized event selection efficiencies as a function of truth MET for events which have all truth decay vertices occurring before...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t23","@type":"Dataset","description":"Parameterized event selection efficiencies as a function of truth MET for events which have the furthest truth decay occurring inside...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t24","@type":"Dataset","description":"Parameterized event selection efficiencies as a function of truth MET for events which have the furthest truth decay occurring after...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t25","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t26","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t27","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t28","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t29","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t30","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t31","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t32","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t33","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t34","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t35","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.78697.v2/t36","@type":"Dataset","description":"Parameterized vertex level efficiencies as a function of number of particles associated to a truth decay vertex, and the vertex...","name":"Table 36"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1630632?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/78697"}],"inLanguage":"en","name":"Search for long-lived, massive particles in events with displaced vertices and missing transverse momentum in $\\sqrt{s}$ = 13 TeV $pp$ collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1630632?version=2","version":2}