{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89322.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1729240"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-7199-0","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"\"Measurements of the $W^+\\rightarrow\\mu^+\\nu$ and $W^-\\rightarrow\\mu^-\\bar{\\nu}$ cross-sections\nand the associated charge asymmetry as a function of the absolute pseudorapidity of the decay muon.\nThe data were collected in proton-proton collisions at a centre-of-mass energy of 8 TeV\nwith the ATLAS experiment at the LHC and correspond to a total integrated luminosity of 20.2 $\\textrm{fb}^{-1}$.\nThe integrated cross-sections for $W^+\\rightarrow\\mu^+\\nu$ and $W^-\\rightarrow\\mu^-\\bar{\\nu}$ production are measured in a fiducial phase space defined \nat the particle level by requiring the muon transverse momentum to be greater than 25 GeV \nand the neutrino transverse momentum to be greater than 25 GeV. \nThe absolute muon pseudorapidity is required to be less than 2.4. \nThe W boson transverse mass must be at least 40 GeV.\nThe differential cross-sections and charge asymmetry are measured in the same fiducial phase space as for the integrated measurement. \nThese are measured in 11 bins of absolute muon pseudorapidity between 0 and 2.4 with bin edges at \n0, 0.21, 0.42, 0.63, 0.84, 1.05, 1.37, 1.52, 1.74, 1.95, 2.18, and 2.4. \nSee 1904.05631 for more details.\"","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t1","@type":"Dataset","description":"The correction factors, $C_{W^\u00b1,i}$ with their associated systematic uncertainties as a function of $|\\eta_{\\mu}|$, for $W^+$ and $W^\u2212$","name":"Table 2a"},{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t2","@type":"Dataset","description":"The integrated global correction factor $C_{W^\u00b1}$, for $W^+$ and $W^\u2212$","name":"Table 2b"},{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t3","@type":"Dataset","description":"Cross-sections (differential in $\\eta_{\\mu}$) and asymmetry, as a function of $|\\eta_{\\mu}|$). The central values are provided along with the statistical...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t4","@type":"Dataset","description":"The measured fiducial production cross-sections times branching ratio for $W^+\\rightarrow\\mu^+\\nu$ and $W^-\\rightarrow\\mu^-\\bar{\\nu}$, their sum, and their ratio for data","name":"Table 4a"},{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t5","@type":"Dataset","description":"The measured fiducial production cross-sections times branching ratio for $W^+\\rightarrow\\mu^+ u$ and $W^-\\rightarrow\\mu^-\\bar{\\nu}$, their sum, and their ratio for the...","name":"Table 4b"},{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t6","@type":"Dataset","description":"Size of the $W^{+}$ the cross-section (differential in $\\eta_{\\mu}$, as a function of $|\\eta_{\\mu}|$. The central values are provided along...","name":"Table 5a"},{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t7","@type":"Dataset","description":"Size of the $W^{+}$ the cross-section (differential in $\\eta_{\\mu}$, as a function of $|\\eta_{\\mu}|$. The central values are provided along...","name":"Table 5b"},{"@id":"https://doi.org/10.17182/hepdata.89322.v1/t8","@type":"Dataset","description":"Size of the asymmetry as a function of $|\\eta_{\\mu}|$. The central values are provided along with the statistical and systematic...","name":"Table 5c"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1729240?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/89322"}],"inLanguage":"en","name":"Measurement of the cross-section and charge asymmetry of $W$ bosons produced in proton-proton collisions at $\\sqrt{s}=8$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1729240?version=1","version":1}