{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.68759.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1382590"}},{"@id":"https://doi.org/10.1016/j.physletb.2016.03.060","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2015","description":"CERN-LHC.  Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.\n\nThe fiducial region is defined as:\n- 4 particle-level jets of at least 30 GeV within $|\\eta| < 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.\n- One electron or muon of $p_\\text{T} > 30 \\, (27) \\, \\text{GeV}$ within $|\\eta| < 2.5 \\,(2.1)$.\n- Reject events with an additional electron or muon of $p_\\text{T} > 20 \\, (10) \\, \\text{GeV}$ within $|\\eta| < 2.5 \\,(2.5)$.\n- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\\Delta R < 0.4$ to the lepton, with $\\Delta R = \\sqrt{ (\\Delta \\eta)^2 + (\\Delta \\phi)^2 }$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t1","@type":"Dataset","description":"Corrected asymmetry as a function of $|y_\\mathrm{t\\bar{t}}|$ in the fiducial phase space. The value 9999 is used as a placeholder...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t2","@type":"Dataset","description":"Correlation matrix for the asymmetries as a function of $|y_\\mathrm{t\\bar{t}}|$ in the fiducial phase space. Both statistical and systematic effects...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t3","@type":"Dataset","description":"Corrected asymmetry as a function of $p_\\text{T}^\\mathrm{t\\bar{t}}$ in the fiducial phase space. The value 9999 is used as a placeholder...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t4","@type":"Dataset","description":"Correlation matrix for the asymmetries as a function of $p_\\text{T}^\\mathrm{t\\bar{t}}$ in the fiducial phase space. Both statistical and systematic effects...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t5","@type":"Dataset","description":"Corrected asymmetry as a function of $m_\\mathrm{t\\bar{t}}$ in the fiducial phase space, using three bins in $m_\\mathrm{t\\bar{t}}$. The value 9999...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t6","@type":"Dataset","description":"Correlation matrix for the asymmetries as a function of $m_\\mathrm{t\\bar{t}}$ in the fiducial phase space, using three bins in $m_\\mathrm{t\\bar{t}}$....","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t7","@type":"Dataset","description":"Corrected asymmetry as a function of $m_\\mathrm{t\\bar{t}}$ in the fiducial phase space, using six bins in $m_\\mathrm{t\\bar{t}}$. The value 9999...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t8","@type":"Dataset","description":"Correlation matrix for the asymmetries as a function of $m_\\mathrm{t\\bar{t}}$ in the fiducial phase space, using six bins in $m_\\mathrm{t\\bar{t}}$....","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t9","@type":"Dataset","description":"Corrected asymmetry as a function of $|y_\\mathrm{t\\bar{t}}|$ in the full phase space. The value 9999 is used as a placeholder...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t10","@type":"Dataset","description":"Correlation matrix for the asymmetries as a function of $|y_\\mathrm{t\\bar{t}}|$ in the full phase space. Both statistical and systematic effects...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t11","@type":"Dataset","description":"Corrected asymmetry as a function of $p_\\text{T}^\\mathrm{t\\bar{t}}$ in the full phase space. The value 9999 is used as a placeholder...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t12","@type":"Dataset","description":"Correlation matrix for the asymmetries as a function of $p_\\text{T}^\\mathrm{t\\bar{t}}$ in the full phase space. Both statistical and systematic effects...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t13","@type":"Dataset","description":"Corrected asymmetry as a function of $m_\\mathrm{t\\bar{t}}$ in the full phase space, using three bins in $m_\\mathrm{t\\bar{t}}$. The value 9999...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t14","@type":"Dataset","description":"Correlation matrix for the asymmetries as a function of $m_\\mathrm{t\\bar{t}}$ in the full phase space, using three bins in $m_\\mathrm{t\\bar{t}}$....","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.68759.v1/t15","@type":"Dataset","description":"Corrected asymmetry as a function of $m_\\mathrm{t\\bar{t}}$ in the full phase space, using six bins in $m_\\mathrm{t\\bar{t}}$. 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