2013
DOI: 10.48550/arxiv.1301.3395
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Predictions for $p+$Pb Collisions at sqrt s_NN = 5 TeV

J. L. Albacete,
N. Armesto,
R. Baier
et al.

Abstract: Predictions for charged hadron, identified light hadron, quarkonium, photon, jet and gauge bosons in p+Pb collisions at √ s N N = 5 TeV are compiled and compared. When test run data are available, they are compared to the model predictions.

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Cited by 42 publications
(57 citation statements)
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“…Multiple scatterings in deeply inelastic lepton-nucleus scattering, hadron-nucleus and heavy-ion collisions lead to many interesting phenomena that in turn can provide useful tools for diagnosing properties of cold and hot nuclear media [1][2][3][4]. The predicted phenomena such as jet quenching and transverse momentum broadening [5][6][7][8][9][10][11][12] have been observed in the fixed target experiments at the Deutsches Elektronen-Synchrotron, Jefferson Lab and Fermilab [13][14][15][16][17][18][19][20], as well as in the ongoing collider experiments at Relativistic Heavy Ion Collider and the Large Hadron Collider [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…Multiple scatterings in deeply inelastic lepton-nucleus scattering, hadron-nucleus and heavy-ion collisions lead to many interesting phenomena that in turn can provide useful tools for diagnosing properties of cold and hot nuclear media [1][2][3][4]. The predicted phenomena such as jet quenching and transverse momentum broadening [5][6][7][8][9][10][11][12] have been observed in the fixed target experiments at the Deutsches Elektronen-Synchrotron, Jefferson Lab and Fermilab [13][14][15][16][17][18][19][20], as well as in the ongoing collider experiments at Relativistic Heavy Ion Collider and the Large Hadron Collider [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…A suppression of the J/ψ production with respect to pp collisions is measured at forward rapidity (y) while at backward y no suppression is found. A fair agreement is seen with models including nuclear shadowing with the EPS09 parameterizations [5,7], and with models including a coherent parton energy loss contribution [11]. For deeper understanding of the CNM effects differential studies are needed.…”
Section: Introductionmentioning
confidence: 66%
“…Initial state effects occur before the cc pair formation (e.g. gluon shadowing [4,5,7] or saturation [8]). Final state effects occur after the cc pair production (e.g.…”
Section: Introductionmentioning
confidence: 99%
“…Various models for prompt J/ψ production are compared to the data. First, a model based on nuclear parton distribution functions (nPDF) EPS09 associated to the Color Evaporation Model (CEM) at NLO [16] for the J/ψ production (shadowing model) reproduces well the rapidity dependence of the suppression. The theoretical uncertainties arise from the EPS09 nPDF and from the mass, the factorization and renormalization scale uncertainties on the cross-section calculation.…”
Section: Quarkonium Measurements In P-pb Collisions Atmentioning
confidence: 99%