{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.73739.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/890503"}},{"@id":"https://doi.org/10.1140/epjc/s10052-011-1557-x","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"DELPHI Collaboration"},"creator":{"@type":"Organization","name":"DELPHI Collaboration"},"datePublished":"2016","description":"CERN-LEP.  The nature of b-quark jet hadronisation has been investigated using data taken at the Z peak by the DELPHI detector at LEP. Two complementary methods are used to reconstruct the energy of weakly decaying b-hadrons, $E^{\\rm weak}_{\\rm B}$. The average value of $x^{\\rm weak}_{\\rm B} = E^{\\rm weak}_{\\rm B}/E_{\\rm beam}$ is measured to be $0.699 \\pm 0.011$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.73739.v1/t1","@type":"Dataset","description":"The combined unfolded and weighted results, per bin, for $f(x^{\\rm weak}_{\\rm B})$. Quoted uncertainties have been scaled by 1.31.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.73739.v1/t2","@type":"Dataset","description":"The average value of the $x^{\\rm weak}_{\\rm B}$ distribution.","name":"Table 2"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins890503?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/73739"}],"inLanguage":"en","name":"A study of the b-quark fragmentation function with the DELPHI detector at LEP I and an averaged distribution obtained at the Z Pole","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins890503?version=1","version":1}