{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.44713.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/421105"}},{"@id":"https://doi.org/10.1007/s002880050281","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"H1 Collaboration"},"creator":{"@type":"Organization","name":"H1 Collaboration"},"datePublished":"1996","description":"DESY-HERA. Measurement of cross sections of charm production and charm contributions to the proton structure function in deep-inelastic positron-proton interactions. Charm events are tagged by D0 and D**- events. Kinematic range covered is Q**2 from 10 to 100 GeV**2, and y from 0.01 to 0.7. Numerical values supplied by K. Daum.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t1","@type":"Dataset","description":"Inclusive D meson production cross sections. The second systematc error represents the model uncertainty.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t2","@type":"Dataset","description":"Inclusive charm meson cross section averaged for the two processes. The second systematc error represents the model uncertainty.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t3","@type":"Dataset","description":"Ratio of cross sections of D0 and D* production.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t4","@type":"Dataset","description":"Normalised and absolute PT distributions. In the absolute cross section the first error includes the independent systematic errors. The first...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t5","@type":"Dataset","description":"Normalised and absolute XD distributions. In the absolute cross section the first error includes the independent systematic errors. The first...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t6","@type":"Dataset","description":"Normalised and absolute PT distributions. In the absolute cross section the first error includes the independent systematic errors. The first...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t7","@type":"Dataset","description":"Normalised and absolute XD distributions. In the absolute cross section the first error includes the independent systematic errors. The first...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t8","@type":"Dataset","description":"Charm contribution to F2.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t9","@type":"Dataset","description":"Charm contribution to F2.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t10","@type":"Dataset","description":"Charm contribution to F2.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.44713.v1/t11","@type":"Dataset","description":"Charm contribution to F2.","name":"Table 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins421105?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/44713"}],"inLanguage":"en","name":"Inclusive D0 and D*+- production in neutral current deep inelastic e p scattering at HERA.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins421105?version=1","version":1}