Abstract:We investigate the rapidity and transverse momentum distributions of the prompt photon production at the CERN LHC energies considering the current perturbative QCD approaches for this scattering process. Namely, we compare the predictions from the usual NLO pQCD calculations to the the color dipole formalism, using distinct dipole cross sections. Special attention is paid to parton saturation models at high energies, which are expected to be important at the forward rapidities in pp collisions ( √ s = 14 TeV) … Show more
“…However, Ref. [25] demonstrates that a large-x correction should be added to consistently describe the prompt photon phenomenology. Therefore, we have multiplied the GBW dipole cross section by a threshold factor (1 − x 2 ) n (with n = 7).…”
Section: Resultsmentioning
confidence: 99%
“…[24]; such an approach includes QCD gluon evolution via the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equation. It should be noticed that, in the color transparency regime, the Hankel integrals can be analytically performed [25]. We will discuss this case in detail when the x T scaling is studied.…”
“…However, Ref. [25] demonstrates that a large-x correction should be added to consistently describe the prompt photon phenomenology. Therefore, we have multiplied the GBW dipole cross section by a threshold factor (1 − x 2 ) n (with n = 7).…”
Section: Resultsmentioning
confidence: 99%
“…[24]; such an approach includes QCD gluon evolution via the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equation. It should be noticed that, in the color transparency regime, the Hankel integrals can be analytically performed [25]. We will discuss this case in detail when the x T scaling is studied.…”
“…It has been shown before [25] that in central rapidities at RHIC and Tevatron, saturation effects do not play a significant role for the measured range of p T . This situation can be changed at the LHC even at midrapidities as the saturation scale is enhanced by a sizable factor.…”
We present results for the low mass Drell-Yan production in proton-proton collisions at the LHC in the color dipole formalism. The DY differential cross sections at √ s = 7 TeV as a function of dilepton rapidity, transverse momentum and invariant mass are discussed. We have imposed kinematical cuts related to the low mass DY production investigated by ATLAS and LHCb collaborations.
“…In next section we introduce the main formulae to compute the hadronic differential cross section. It is already known from previous studies [7] that the photon transverse momentum spectrum is a sensitive probe of color dipole scattering cross section. We investigate the consequence of using several implementations of dipole cross sections which are constrained from deep inelastic scattering data.…”
Section: Introductionmentioning
confidence: 99%
“…Their interaction with the medium is purely electromagnetic, which gives a baseline for the interpretation of jetquenching models. From the theoretical point of view, the prompt photon production is reasonably described in the next-to-leading order (NLO) perturbative QCD (pQCD) approach [1] and on the color dipole formalism [2][3][4][5][6][7] as well. Recently, the first measurements of inclusive photon production in association with heavy flavour jets have been reported by D0 Collaboration [8].…”
We apply the target rest frame formalism to photon þ heavy quark production cross section in hadronic collisions at high energies. We investigate the dependence of the production cross section on the photon and quark rapidities and transverse momenta. It is shown that the photon transverse momentum spectrum is a sensitive probe of color dipole scattering amplitude. The theoretical results are compared to Tevatron measurements of the differential þ c þ X and þ b þ X production cross sections at ffiffi ffi s p ¼ 1:96 TeV.An analysis for proton-proton and proton-lead collisions at the LHC regime is also performed.
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