{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.61422.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1234228"}},{"@id":"https://doi.org/10.1016/j.physletb.2013.07.049","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2013","description":"CERN-LHC. Based on an integrated luminosity of 4.9 /fb, the differential cross-section in the Z/gamma* to e+e- channel is measured with the ATLAS detector as a function of the invariant mass, Mee, in the range 116 &lt; Mee &lt; 1500 GeV, for a fiducial region in which both the electron and the positron have transverse momentum pT &gt; 25 GeV and absolute pseudorapidity |eta| &lt; 2.5.\nNote that based on the update of the ATLAS Luminosity measurement (Eur.Phys.J. C73 (2013) 2518) the measured cross-sections given here and in the paper need to be scaled up by 1.4%. The luminosity uncertainty stays at the previous value of 1.8%.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.61422.v1/t1","@type":"Dataset","description":"Measured differential cross sections as a function of the di-electron mass for DY production at the Born and dressed levels.","name":"Table 1"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1234228?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/61422"}],"inLanguage":"en","name":"Measurement of the high-mass Drell--Yan differential cross-section in pp collisions at sqrt(s)=7 TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1234228?version=1","version":1}
