Measurement of the cross section for direct-photon production in association with a heavy quark in $p\bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV

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A cylindrical coordinate system, ( r , ϕ , z ) (r,\phi,z) is used with origin at the geometric center of the detector; r r is the radius from the nominal beam line, ϕ \phi is the azimuthal angle, and + z +z points along the direction of the proton beam. The polar angle θ \theta with respect to the proton beam defines the pseudorapidity η \eta , which is given by η = − ln ⁡ [ tan ⁡ ( θ / 2 ) ] \eta=-\ln[\tan(\theta/2)] . Transverse energy and transverse momentum are defined as E T = E sin ⁡ ( θ ) E_{T}=E\sin(\theta) and p T = p sin ⁡ ( θ ) p_{T}=p\sin(\theta) , respectively
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