{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.81690.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1635271"}},{"@id":"https://doi.org/10.1007/JHEP03(2018)115","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"The kinematic variables\ndescribe the $\\ell$+jets, where $\\ell$ can be either a muon ($\\mu$)\nor electron ($\\rm{e}$), and the dilepton ($\\rm{e}^\\pm \\mu^\\mp$ or $\\mu^\\pm \\mu^\\mp$) decay channels.\nThe measured cross sections are given per decay channel and for their combination.\n\nThe fiducial region in the $\\ell$+jets decay channel is defined as:\n- $\\equiv$1$\\rm{e}$($\\mu$), $p_T$>35(25)GeV&&|$\\eta$|<2.1\n- including the transition 1.444<|$\\eta$|<1.566 region in the $\\rm{e}$+jets channel\n- no additional lepton with $p_T$>15GeV&&|$\\eta$|<2.5 and $p_T$>10GeV&&|$\\eta$|<2.5 in the $\\mu$+jets and $\\rm{e}$+jets channel, respectively\n- $\\geq$2jets(anti-kt,R=0.4), $p_T$>25GeV&&|$\\eta$|<2.4\n- min($\\Delta R(jet,\\ell)$) > 0.3\n- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\\Delta R(j,j')$, where $\\Delta R=\\sqrt{ (\\Delta \\eta)^{2} + (\\Delta \\phi)^{2}}$\n\nThe acceptance is measured in the $\\ell$+jets channel as:\n0.301$\\pm$0.007(tot)\n\nThe fiducial region in the dilepton decay channel is defined as:\t\n- $\\geq1\\rm{e}$ or $\\mu$ with $p_T$>20GeV&&|$\\eta$|<2.4 and $p_T$>18GeV&&|$\\eta$|<2.1, respectively\n- including the transition 1.444<|$\\eta$|<1.566 region for electrons\n- $\\geq$2jets(anti-kt,R=0.4), $p_T$>25GeV&&|$\\eta$|<3.0\n- min($\\Delta R(jet,\\ell)$) > 0.3\n- $M_{\\ell \\ell}$ > 20 GeV\n- 76 <$M_{\\ell \\ell}$ < 106 GeV and $p_{\\rm{T}}^{\\rm{mss}}$>35 GeV only in the  $\\mu^\\pm \\mu^\\mp$ channel\n- ambiguities in forming the candidate pair are resolved by selecting the two leptons of opposite charge that yield the highest scalar $p_T$ sum\n\nThe acceptance is measured in the dilepton channel as:\n0.53$\\pm$0.01(tot) in the $\\rm{e}^\\pm \\mu^\\mp$ and  0.37$\\pm$0.01(tot) in the $\\mu^\\pm \\mu^\\mp$ channel, respectively\n\nThe efficiency is measured in the dilepton channel as:\n0.55$\\pm$0.02(tot) in the $\\rm{e}^\\pm \\mu^\\mp$ and  0.57$\\pm$0.04(tot) in the $\\mu^\\pm \\mu^\\mp$ channel, respectively\n\nIn both the $\\ell$+jets and dilepton analyses, events with $\\tau$ leptons are considered as signal if they decay to electrons or muons that satisfy the selection requirements, and are included in the simulation.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t1","@type":"Dataset","description":"The measured fiducial cross sections in the $\\ell$+jets and dilepton ($\\rm{e}^\\pm \\mu^\\mp$ or $\\mu^\\pm \\mu^\\mp$) decay channels. The first uncertainty...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t2","@type":"Dataset","description":"The measured total cross sections based on the $\\ell$+jets (left), $\\rm{e}^\\pm \\mu^\\mp$ (middle) and $\\mu^\\pm \\mu^\\mp$ (right) decay channels. The...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t3","@type":"Dataset","description":"The measured total cross section in the combined $\\ell$+jets and dilepton ($\\rm{e}^\\pm \\mu^\\mp$ or $\\mu^\\pm \\mu^\\mp$) decay channels. The weights...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t4","@type":"Dataset","description":"The observed distribution of the dijet invariant mass in the $\\ell$+jets decay channel in the 0 b tagged jet category....","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t5","@type":"Dataset","description":"The observed distribution of the dijet invariant mass in the $\\ell$+jets decay channel in the 1 b tagged jet category....","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t6","@type":"Dataset","description":"The observed distribution of the dijet invariant mass in the $\\ell$+jets decay channel in the $\\geq$2 b tagged jet category....","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t7","@type":"Dataset","description":"The observed distribution of the the minimum angular distance $\\Delta R$ between all pairs of jets $j$ and $j'$ in...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t8","@type":"Dataset","description":"The observed distribution of the the minimum angular distance $\\Delta R$ between all pairs of jets $j$ and $j'$ in...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t9","@type":"Dataset","description":"The observed distribution of the the minimum angular distance $\\Delta R$ between all pairs of jets $j$ and $j'$ in...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t10","@type":"Dataset","description":"The observed distribution of the jet multiplicity in the $\\rm{e}^\\pm \\mu^\\mp$ decay channel for events passing the dilepton criteria. The...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t11","@type":"Dataset","description":"The observed distribution of the scalar $p_{\\rm{T}}$ sum of all jets in the $\\rm{e}^\\pm \\mu^\\mp$ decay channel for events passing...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t12","@type":"Dataset","description":"The observed distribution of the invariant mass of the lepton pair in the $\\rm{e}^\\pm \\mu^\\mp$ decay channel after requiring at...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t13","@type":"Dataset","description":"The observed distribution of the $p_{\\rm{T}}$ of the lepton pair in the $\\rm{e}^\\pm \\mu^\\mp$ decay channel after requiring at least...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t14","@type":"Dataset","description":"The observed distribution of the $p_{\\rm{T}}^{\\rm{miss}}$ in the $\\mu^\\pm \\mu^\\mp$ decay channel for events passing the dilepton criteria and Z...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.81690.v1/t15","@type":"Dataset","description":"The observed distribution of the invariant mass of the lepton pair in the $\\mu^\\pm \\mu^\\mp$ decay channel for events passing...","name":"Table 15"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1635271?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/81690"}],"inLanguage":"en","name":"Measurement of the inclusive $\\mathrm{t}\\overline{\\mathrm{t}}$ cross section in pp collisions at $\\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1635271?version=1","version":1}