2004
DOI: 10.1016/j.nuclphysa.2004.07.006
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High energy pA collisions in the color glass condensate approach II: quark pair production

Abstract: We compute the production of quark-antiquark pairs in high energy collisions between a small and a large projectile, as in proton-nucleus collisions, in the framework of the Color Glass Condensate. We derive a general expression for quark pair-production, which is not k ⊥ -factorizable. However, k ⊥ -factorization is recovered in the limit of large mass pairs or large quark-anti-quark momenta. Our results are amenable to a simple interpretation and suggest how multi-parton correlations at small x can be quanti… Show more

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Cited by 264 publications
(396 citation statements)
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References 47 publications
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“…Consider for instance, one of the tree subdiagrams contained in eq. (58). Summing over the + or − indices of the "leaves" (or "blobs") of the tree, the outer layer of propagators is transformed into retarded propagators, thanks to eqs.…”
Section: Leading Order Resultsmentioning
confidence: 99%
“…Consider for instance, one of the tree subdiagrams contained in eq. (58). Summing over the + or − indices of the "leaves" (or "blobs") of the tree, the outer layer of propagators is transformed into retarded propagators, thanks to eqs.…”
Section: Leading Order Resultsmentioning
confidence: 99%
“…In this Gaussian approximation, one can compute the 2-point, 3-point and 4-point correlators in closed form [38,88,89,54,55,56,90, 1] -see Appendix A of ref. [1] for the explicit expressions for arbitrary N . We quote here the large N limits for these correlators because only these are used in the discussion of the energy evolution of correlators 13 :…”
Section: Correlators In the MV Modelmentioning
confidence: 99%
“…[1]. A full treatment of multiple scattering and quantum evolution effects at high energies requires a computation of the previously mentioned 2-point, 3-point and 4-point correlation functions as a function of x, or of the rapidity Y (= ln(1/x)).…”
Section: Introductionmentioning
confidence: 99%
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“…Regarding the initial saturation scale, we choose Q 2 s0,A = 3Q 2 s0,p for the heavy nuclei, Au and Pb. 4 As to the transverse radius of the nucleus, we determine it by imposing the nuclear modification factor R pA = 1 at high p ⊥ . The results obtained by Eq.…”
Section: Pa Collisions and Nuclear Modification Factormentioning
confidence: 99%