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We present measurements of the differential cross section dsigma/dpT_gamma for the inclusive production of a photon in association with a b-quark jet for photons with rapidities |y_gamma|< 1.0 and 30<pT_gamma <300 GeV, as well as for photons with 1.5<|y_gamma|< 2.5 and 30< pT_gamma <200 GeV, where pT_gamma is the photon transverse momentum.
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The polar angle θ \theta and the azimuthal angle ϕ \phi are defined with respect to the positive z z axis, which is along the proton beam direction. Pseudorapidity is defined as η = − ln [ tan ( θ / 2 ) ] \eta=-\ln[\tan(\theta/2)] . Also, η det \eta_{\text{det}} and ϕ det \phi_{\text{det}} are the pseudorapidity and the azimuthal angle measured with respect to the center of the detector
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The primary p p ¯ p\bar{p} interaction vertex is that found to be the most likely collision point, among possibly several collisions within a specific beam crossing, from which our selected objects emanate. The algorithm for defining it can be found in [9]
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