2010
DOI: 10.1016/j.physletb.2010.02.073
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Single inclusive hadron production at RHIC and the LHC from the color glass condensate

Abstract: Using the unintegrated gluon distribution obtained from numerical simulations of the Balitsky-Kovchegov equation with running coupling, we obtain a very good description of RHIC data on single inclusive hadron production at forward rapidities in both p+p and d+Au collisions. No K-factors are needed for charged hadrons, whereas for pion production a rapidity independent K-factor of order 1/3 is needed. Extrapolating to LHC energies, we calculate nuclear modification factors for light hadrons in p+Pb collision, … Show more

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Cited by 189 publications
(296 citation statements)
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“…The main purpose of this paper is to explore to what extent this disagreement stems from the framework itself, and how much is due to approximations concerning nuclear geometry that are necessary for relating the CGC description of the proton to that of the nucleus. Indeed, in the case of single inclusive light hadron production [8], the disagreement with early CGC nuclear suppression calculations [26] and LHC data turned out to be mostly due to the nuclear geometry effects. We will in this paper calculate cross sections for inclusive (prompt) forward J/ψ production in proton-proton and proton-nucleus collisions using the collinear "hybrid" framework also used in Ref.…”
Section: Introductionmentioning
confidence: 96%
“…The main purpose of this paper is to explore to what extent this disagreement stems from the framework itself, and how much is due to approximations concerning nuclear geometry that are necessary for relating the CGC description of the proton to that of the nucleus. Indeed, in the case of single inclusive light hadron production [8], the disagreement with early CGC nuclear suppression calculations [26] and LHC data turned out to be mostly due to the nuclear geometry effects. We will in this paper calculate cross sections for inclusive (prompt) forward J/ψ production in proton-proton and proton-nucleus collisions using the collinear "hybrid" framework also used in Ref.…”
Section: Introductionmentioning
confidence: 96%
“…This normalization uncertainty cancels out in R pA , the ratio of proton-nucleus and proton-proton cross sections, corrected by the nuclear geometry. Since other uncertainties in R pA are rather small, it is important to treat the nuclear geometry correctly also in the theory calculations, indeed the largest difference between earlier [15] and more recent [14] calculations is precisely here. In a similar way the importance of treating carefully the nuclear geometry has been seen in calculations of J/Ψ production at forward rapidity [18,19].…”
Section: Control Measurementsmentioning
confidence: 95%
“…Here the particle production cross section is proportional to the nuclear unintegrated gluon distribution, which is given simply by a Fourier-transform of the dipole cross section. Leading order calculations with up-to-date dipole cross sections now give a relatively good description of the spectra, albeit with the normalization corrected by a "K-factor" [14][15][16][17]. This normalization uncertainty cancels out in R pA , the ratio of proton-nucleus and proton-proton cross sections, corrected by the nuclear geometry.…”
Section: Control Measurementsmentioning
confidence: 98%
“…The LO contribution together with some running coupling effects has been studied quite extensively [20][21][22][23][24].…”
Section: Inclusive Forward Hadron Productions In Pa Collisionsmentioning
confidence: 99%