{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.44587.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/445116"}},{"@id":"https://doi.org/10.1016/S0550-3213(97)00585-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"H1 Collaboration"},"creator":{"@type":"Organization","name":"H1 Collaboration"},"datePublished":"1997","description":"DESY-HERA. Study of the evolution of charged particle fragmentation functions and multiplicity distributions in the & apos;current& apos; hemisphere of the Breit framein deep inelastic scattering of 27.5 GeV positrons on 820 GeV protons.. Numerical values supplied by D Kant.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t1","@type":"Dataset","description":"The current hemisphere fragmentation as a function of XP in the Breit frame.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t2","@type":"Dataset","description":"The current hemisphere fragmentation as a function of LN(1/XP) in the Breitframe.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t3","@type":"Dataset","description":"Current hemisphere fragmentation as a function of Q for the XP range 0.02 to 0.05, to show scaling violations.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t4","@type":"Dataset","description":"Current hemisphere fragmentation as a function of Q for the XP range 0.05 to 0.10, to show scaling violations.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t5","@type":"Dataset","description":"Current hemisphere fragmentation as a function of Q for the XP range 0.10 to 0.20, to show scaling violations.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t6","@type":"Dataset","description":"Current hemisphere fragmentation as a function of Q for the XP range 0.20 to 0.30, to show scaling violations.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t7","@type":"Dataset","description":"Current hemisphere fragmentation as a function of Q for the XP range 0.30 to 0.40, to show scaling violations.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t8","@type":"Dataset","description":"Current hemisphere fragmentation as a function of Q for the XP range 0.40 to 0.50, to show scaling violations.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t9","@type":"Dataset","description":"Current hemisphere fragmentation as a function of Q for the XP range 0.40 to 0.50, to show scaling violations.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t10","@type":"Dataset","description":"The average charged multiplicity, and the peak and width of the fragmentation function (in LN(1/XP)) as a function of the...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t11","@type":"Dataset","description":"The average charged multiplicity, and the peak and width of the fragmentation function (in LN(1/XP)) as a function of the...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t12","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for a mean Q of 5.5. Results are given for all...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t13","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for a mean Q of 19.6. Results are given for all...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t14","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 12 to 15 GeV**2.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t15","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 15 to 20 GeV**2.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t16","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 20 to 40 GeV**2.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t17","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 40 to 60 GeV**2.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t18","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 60 to 80 GeV**2.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t19","@type":"Dataset","description":"Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 80 to 100 GeV**2.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t20","@type":"Dataset","description":"The probability per event of observing a charged hadronic multiplicity of (ULT) in the current hemisphere of the Breit frame...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t21","@type":"Dataset","description":"The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t22","@type":"Dataset","description":"The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t23","@type":"Dataset","description":"The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t24","@type":"Dataset","description":"The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.44587.v1/t25","@type":"Dataset","description":"The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame...","name":"Table 25"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins445116?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/44587"}],"inLanguage":"en","name":"Evolution of e p fragmentation and multiplicity distributions in the Breit frame.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins445116?version=1","version":1}