{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.78567.v1/t3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1310835"}},{"@id":"https://doi.org/10.1016/j.physletb.2014.09.054","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"Measured differential fiducial cross sections in m34, which corresponds to the invariant mass of the off-shell Z boson (second column)....","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/141199/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/141199/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/141199/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/141199/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/141199/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1310835?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/78567"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.78567.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1310835?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.78567.v1","@type":"Dataset","description":"CERN-LHC. Measurements of fiducial and differential cross sections of Higgs boson production in the H->ZZ*->4l channel in  proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012.  The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons.\n\n\nThe 4l channel fiducial region is defined as:\n- 4e, 4mu or 2e2mu\n- ptElectron > 7 GeV, ptMuon > 6 GeV\n- |etaElectron| < 2.47, |etaMuon| < 2.7\n- Ambiguities in pairing are resolved by choosing as the leading same flavor opposite sign pair m12 the one that minimizes |mll - mZ|, and as the second leading pair m34 the remaining one that minimizes |mll - mZ|\n- at least one lepton with each 20, 15, 10 GeV\n- mass requirements 50 GeV < m12 < 106 GeV, 12 GeV < m34 < 115 GeV\n- min(DeltaR(l,l)) > 0.1 (0.2) for same flavor (opposite flavor) lepton pairs\n- Jpsi veto: mll > 5 GeV for all same flavor opposite sign pairs\n- m4l requirement: 118 GeV < m4l < 129 GeV","name":"Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in $pp$ collisions at $\\sqrt{s}$=8 TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1310835?version=1"},"keywords":"P P --> Z0 Z0 X, SIG, 8000.0, Differential Cross Section, Cross Section, Proton-Proton Scattering, Higgs production, m34, four lepton, 4l","name":"Table 3","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/80006","version":1}