{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77020.v1/t3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1408878"}},{"@id":"https://doi.org/10.1016/j.nuclphysb.2016.04.032","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"The measured differential cross sections $\\rm{d}\\sigma/\\rm{d}|\\eta|$ of $D^{*\\pm}$ and $D^\\pm$ production with $3.5<p_T<20\\,$GeV. The first and second errors are the...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/74589/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/74589/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/74589/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/74589/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/74589/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1408878?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77020"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.77020.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1408878?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.77020.v1","@type":"Dataset","description":"CERN-LHC.  The production of $D^{*\\pm}$, $D^\\pm$ and $D_s^\\pm$ charmed mesons has been measured with the ATLAS detector in $pp$ collisions at $\\sqrt{s}=7$ TeV at the LHC, using data corresponding to an integrated luminosity of $280\\,$nb$^{-1}$. The charmed mesons have been reconstructed in the range of transverse momentum $3.5<p_{\\rm T}(D)<100$ GeV and pseudorapidity $|\\eta(D)|<2.1$. The differential cross sections as a function of transverse momentum and pseudorapidity were measured for $D^{*\\pm}$ and $D^\\pm$ production. The next-to-leading-order QCD predictions are consistent with the data in the visible kinematic region within the large theoretical uncertainties. Using the visible $D$ cross sections and an extrapolation to the full kinematic phase space, the strangeness-suppression factor in charm fragmentation, the fraction of charged non-strange $D$ mesons produced in a vector state, and the total cross section of charm production at $\\sqrt{s}=7$ TeV were derived.","name":"Measurement of $D^{*\\pm}$, $D^\\pm$ and $D_s^\\pm$ meson production cross sections in $pp$ collisions at $\\sqrt{s}=7$ TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1408878?version=1"},"keywords":"P P --> D*(2010)+ X, P P --> D*(2010)- X, P P --> D+ X, P P --> D- X, DSIG/DETARAP, Inclusive, Differential Cross Section, Pseudorapidity Dependence, Proton-Proton Scattering, Charm Production, 7000.0","name":"Table 3","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/77030","version":1}