{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.49090.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/792812"}},{"@id":"https://doi.org/10.1016/j.physletb.2008.09.060","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"D0 Collaboration"},"creator":{"@type":"Organization","name":"D0 Collaboration"},"datePublished":"2008","description":"Fermilab-Tevatron. Measurement of the differential cross section for Z0/GAMMA* JET X production in PBAR P collisions at centre of mass energy 1.96 TeV. The data were taken from April 2002 to February 2006 and have a total integrated luminosity of 0.97 +- 0.06 fb-1. The Z0/GAMMA* was measured through its MU+ MU- decay in the region of di-muon mass 65 to 115 GeV and ABS(rapidity) < 1.7 in which it is almost pure Z0 production. Jets are defined using the D0 RunII midpoint cone algorithm with DeltaR = 0.5.     Also given here are the normalised cross sections, calculated by dividing  the absolute cross section by the measured total cross section, 118 pb.  Note that this does suffer from the 8 PCT overall systematic error coming from the  luminsoity, trigger and muon identification uncertainties.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.49090.v1/t1","@type":"Dataset","description":"Measured cross section as a function of the jet transverse momentum.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.49090.v1/t2","@type":"Dataset","description":"Measured cross section as a function of the jet rapidity.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.49090.v1/t3","@type":"Dataset","description":"Measured cross section as a function of the Z0 transverse momentum.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.49090.v1/t4","@type":"Dataset","description":"Measured cross section as a function of the Z0 rapidity.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.49090.v1/t5","@type":"Dataset","description":"Integrated cross section.. The second DSYS error is from the muon identification and the third from the luminosity measurement.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.49090.v1/t6","@type":"Dataset","description":"Measurement of the cross section for inclusive Z0/GAMMA* production. The second DSYS error is from the muon identification and the...","name":"Table 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins792812?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/49090"}],"inLanguage":"en","name":"Measurement of differential Z / gamma* + jet + X cross sections in p anti-p collisions at s**(1/2) = 1.96-TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins792812?version=1","version":1}