{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.60422.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1204447"}},{"@id":"https://doi.org/10.1103/PhysRevD.87.052002","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2013","description":"CERN-LHC. Measurement of the properties of events with 3 or more charged leptons produced in proton-proton  collisions at a centre-of-mass energy of 7 TeV.  The data sample used has a total integrated luminosity  of 4.6 fb-1 collected in 2011.  The events are required to contain at least two electrons or muons, while the  third lepton can be either an additional electron or muon, or a hadronically decaying tau lepton.  Events are  catagorized by the presence or absence of a reconstructed tau-lepton or a Z-boson candidate decaying into leptons.  As well as the fiducial efficiencies the resuts are given as upper limits on event yields from non-SM processes  producing at least 3 prompt, isolated leptons, given as functions of the lower bounds on several   kinematic variables.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t1","@type":"Dataset","description":"The fiducial efficiency for electrons and taus in different pT ranges. For tau candidates, p_T=p_T^vis.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t2","@type":"Dataset","description":"The fiducial efficiency for electrons and taus in different eta ranges. For tau candidates, eta=eta^vis.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t3","@type":"Dataset","description":"The fiducial efficiency for muons in different p_T ranges.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t4","@type":"Dataset","description":"Results for the H_T^leptons signal regions for the &gt;= 3 e/mu off-Z events. Irreducible sources include all backgrounds estimated with...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t5","@type":"Dataset","description":"Results for the H_T^leptons signal regions for the 2 e/mu + &gt;= 1 tau_had off-Z events. Irreducible sources include all...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t6","@type":"Dataset","description":"Results for the H_T^leptons signal regions for the &gt;= 3 e/mu on-Z events. Irreducible sources include all backgrounds estimated with...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t7","@type":"Dataset","description":"Results for the H_T^leptons signal regions for the 2 e/mu + &gt;= 1 tau_had on-Z events. Irreducible sources include all...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t8","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&lt;100 GeV signal regions for the &gt;= 3 e/mu off-Z events. Irreducible sources include all backgrounds...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t9","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&lt;100 GeV signal regions for the 2 e/mu + &gt;= 1 tau_had off-Z events. Irreducible sources...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t10","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&lt;100 GeV signal regions for the &gt;= 3 e/mu on-Z events. Irreducible sources include all backgrounds...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t11","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&lt;100 GeV signal regions for the 2 e/mu + &gt;= 1 tau_had on-Z events. Irreducible sources...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t12","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&gt;=100 GeV signal regions for the &gt;= 3 e/mu off-Z events. Irreducible sources include all backgrounds...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t13","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&gt;=100 GeV signal regions for the 2 e/mu + &gt;= 1 tau_had off-Z events. Irreducible sources...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t14","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&gt;=100 GeV signal regions for the &gt;= 3 e/mu on-Z events. Irreducible sources include all backgrounds...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t15","@type":"Dataset","description":"Results for the E_T^miss, H_T^jets&gt;=100 GeV signal regions for the 2 e/mu + &gt;= 1 tau_had on-Z events. Irreducible sources...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t16","@type":"Dataset","description":"Results for the m_eff signal regions for the &gt;= 3 e/mu off-Z events. Irreducible sources include all backgrounds estimated with...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t17","@type":"Dataset","description":"Results for the m_eff signal regions for the 2 e/mu + &gt;= 1 tau_had off-Z events. Irreducible sources include all...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.60422.v1/t18","@type":"Dataset","description":"Results for the m_eff signal regions for the &gt;= 3 e/mu on-Z events. 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