{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.52513.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/826756"}},{"@id":"https://doi.org/10.1016/j.physletb.2009.11.012","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"D0 Collaboration"},"creator":{"@type":"Organization","name":"D0 Collaboration"},"datePublished":"2009","description":"Fermilab-Tevatron. Measurement of differential cross sections for  Z/GAMMA* + JET +X production in PBAR P collisions at a centre-of-mass energy of 1.96 TeV.  Data are presented in bins of the azimuthal angle between the  Z/GAMMA* (P=3) and the leading jet (P=4), the absolute value of the rapidity difference between the Z/GAMMA* and the leading jet and the absolute value of the average rapidity of the Z/GAMMA* and the leading jet, all  normalised to the inclusive Z/GAMMA* production cross section. Data are presented for  two minimum values of the Z/GAMMA* transverse momentum. The data were  collected during the period from April 2002 to February 2006 and have a  total integrated luminsoity of 0.97 +- 0.06 fb-1. This record also contains, at the request of the authors, the absolute cross sections obtained by multiplying by the measured total inelastic cross section od 118 PB. This also introduces an 8% overall normalization error     The systematic (DSYS) error in the first 6 tables is the total  systematic error including both uncorrelated and correlated sources. The later tables give the percentage systematic errors from the individual different sources where the  errors from sources 1-10 are correlated across all bins and all distributions.  The sources of systematic error are:    0: Uncorrelated systematic error.    1: del(phi),del(y) and y re-weighting.    2: Jet y re-weighting.    3: Z0/GAMMA* re-weighting.    4: Jet PT re-weighting.    5: Data overlay on simulation.    6: Muon 1/PT resolution.    7: Muon identification efficiency.    8: Jet identification efficiency.    9: Jet energy resolution.    10: Jet energy scale.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t1","@type":"Dataset","description":"Differential cross section in bins of PHI(P=3)-PHI(P=4) for Z/GAMMA* transverse momentum > 25 GeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t2","@type":"Dataset","description":"Differential cross section in bins of PHI(P=3)-PHI(P=4) for Z/GAMMA* transverse momentum > 45 GeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t3","@type":"Dataset","description":"Differential cross section in bins of ABS(YRAP(P=3)-YRAP(P=4)) for Z/GAMMA* transverse momentum > 25 GeV.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t4","@type":"Dataset","description":"Differential cross section in bins of ABS(YRAP(P=3)-YRAP(P=4)) for Z/GAMMA* transverse momentum > 45 GeV.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t5","@type":"Dataset","description":"Differential cross section in bins of ABS(YRAP(P=3)+YRAP(P=4))/2 for Z/GAMMA* transverse momentum > 25 GeV.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t6","@type":"Dataset","description":"Differential cross section in bins of ABS(YRAP(P=3)+YRAP(P=4))/2 for Z/GAMMA* transverse momentum > 45 GeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t7","@type":"Dataset","description":"Individual percentage contributions to the systematic error for the binning in PHI(P=3)-PHI(P=4) for Z/GAMMA* transverse momentum > 25 GeV.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t8","@type":"Dataset","description":"Individual percentage contributions to the systematic error for the binning in PHI(P=3)-PHI(P=4) for Z/GAMMA* transverse momentum > 45 GeV.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t9","@type":"Dataset","description":"Individual percentage contributions to the systematic error for the binning in ABS(YRAP(P=3)-YRAP(P=4)) for Z/GAMMA* transverse momentum > 25 GeV.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t10","@type":"Dataset","description":"Individual percentage contributions to the systematic error for the binning in ABS(YRAP(P=3)-YRAP(P=4)) for Z/GAMMA* transverse momentum > 45 GeV.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t11","@type":"Dataset","description":"Individual percentage contributions to the systematic error for the binning in ABS(YRAP(P=3)+YRAP(P=4))/2 for Z/GAMMA* transverse momentum > 25 GeV.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.52513.v1/t12","@type":"Dataset","description":"Individual percentage contributions to the systematic error for the binning in ABS(YRAP(P=3)+YRAP(P=4))/2 for Z/GAMMA* transverse momentum > 45 GeV.","name":"Table 12"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins826756?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/52513"}],"inLanguage":"en","name":"Measurement of $Z / \\gamma^\\ast +jet+X$ angular distributions in $p \\bar{p}$ collisions at $\\sqrt{s}=1.96$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins826756?version=1","version":1}