{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.42780.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/682179"}},{"@id":"https://doi.org/10.1103/PhysRevD.71.112002","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CDF Collaboration"},"creator":{"@type":"Organization","name":"CDF Collaboration"},"datePublished":"2005","description":"Fermilab-Tevatron. Measurement of the differential and integral jet shapes for inclusive jet production in PBAR P collisions at centre of mass energy 1.96 TeV. The data are taken with the upgrade CDF detector in RUN-II and have a totalintegrated luminosity 170 pb-1 over the absolute jet rapidity region 0.1 to 0.7 and jet transverse momentum from 37 to380 GeV. The differential jet shape RHO(R)is defined as the average fraction of the jet transverse momentum inside an annulus of inner(outer) radius R - DELTAR/2 (R + DELTAR/2), where R = SQRT(DY**2+ DPHI**2). The integrated jet shape PSI(R) is defined as the average fraction of the jet transverse momentum inside a cone of radius R concentric to the jet cone. Jets are defined with a jet cone parameter R = R0 = 0.7.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t1","@type":"Dataset","description":"The measured differential jet shape.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t2","@type":"Dataset","description":"The measured differential jet shape.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t3","@type":"Dataset","description":"The measured differential jet shape.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t4","@type":"Dataset","description":"The measured differential jet shape.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t5","@type":"Dataset","description":"The measured differential jet shape.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t6","@type":"Dataset","description":"The measured differential jet shape.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t7","@type":"Dataset","description":"The measured integrated jet shape.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t8","@type":"Dataset","description":"The measured integrated jet shape.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t9","@type":"Dataset","description":"The measured integrated jet shape.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t10","@type":"Dataset","description":"The measured integrated jet shape.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t11","@type":"Dataset","description":"The measured integrated jet shape.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t12","@type":"Dataset","description":"The measured integrated jet shape.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.42780.v1/t13","@type":"Dataset","description":"The measured integrated cross section for R = 0.3 as a function of the meanPT.","name":"Table 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins682179?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/42780"}],"inLanguage":"en","name":"Study of jet shapes in inclusive jet production 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/ins682179?version=1","version":1}