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We present measurements of the differential cross section $d\sigma/dp_{T}^{\gamma}$ for the associated production of a $c$-quark jet and an isolated photon with rapidity $|y^{\gamma}|< 1.0$ and transverse momentum $30 < p_{T}^{\gamma} < 300$ GeV.
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The rapidity y y is related to the polar scattering angle θ \theta with respect to the proton beam axis by y = 0.5 ln [ ( 1 + β cos θ ) / ( 1 − β cos θ ) ] y=0.5\ln[(1+\beta\cos\theta)/(1-\beta\cos\theta)] , where β \beta is defined as the ratio between momentum and energy β = | p → | / E \beta=|\vec{p}|/E
Cited in the paper.
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}} is the pseudorapidity measured with respect to the center of the detector
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The primary p p ¯ p\bar{p} interaction vertex is the most likely hard collision point, among possibly several collisions within a specific beam crossing. The algorithm for defining primary vertex can be found in [ 3 ]
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2012
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