{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.76740.v1/t4","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1397632"}},{"@id":"https://doi.org/10.1103/PhysRevD.93.032006","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"Belle Collaboration"},"creator":{"@type":"Organization","name":"Belle Collaboration"},"datePublished":"2017","description":"The correlation matrix of the systematic error. The value of $w_\\rm{max} = 1.59055$ is the average of the values for...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/320032/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/320032/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/320032/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/320032/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/320032/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1397632?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/76740"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.76740.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1397632?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.76740.v1","@type":"Dataset","description":"KEK-BF. We present a determination of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ using the decay $B\\to D\\ell\\nu_\\ell$ ($\\ell=e,\\mu$) based on 711 fb$^{-1}$ of $e^+e^-\\to \\Upsilon(4S)$ data recorded by the Belle detector and containing $772 \\times 10^6$ $B\\bar{B}$ pairs. One $B$ meson in the event is fully reconstructed in a hadronic decay mode while the other, on the signal side, is partially reconstructed from a charged lepton and either a $D^+$ or $D^0$ meson in a total of 23 hadronic decay modes. The isospin-averaged branching fraction of the decay $B\\to D\\ell\\nu_\\ell$ is found to be $\\mathcal{B}(B^0 \\to D^- \\ell^+ \\nu_{\\ell})=(2.31\\pm 0.03(\\mathrm{stat})\\pm 0.11(\\mathrm{syst}))\\%$.\n\nUPDATE (23 FEB 2017): split Table 1 from paper into two data tables so that $w_\\rm{max}$ can be replaced by the numerical value (different for charged and neutral $B$ mesons).","name":"Measurement of the decay $B\\to D\\ell\\nu_\\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$","url":"https://www.hepdata.net/record/ins1397632?version=1"},"keywords":"B0 --> D- E+ NUE, B0 --> D- MU+ NUMU, B+ --> DBAR0 E+ NUE, B+ --> DBAR0 MU+ NUMU, WIDTH, Decay, Charm Production, Muon Production, Electron Production","name":"Table 4","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/76744","version":1}