Multi-particle production in proton–nucleus collisions in the color glass condensate

Abstract We compute multi-gluon production in the Color Glass Condensate approach in dilute-dense collisions, $$\hbox {p}A$$ p A , extending previous calculations up to four gluons. We include the contributions that are leading in the overlap area of the collision but keep all orders in the expansio...

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Main Authors: Pedro Agostini, Tolga Altinoluk, Néstor Armesto
Format: Article
Language:English
Published: SpringerOpen 2021-08-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-021-09475-0
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spelling doaj-02ff7b9befec44cdb37fc0d86402934b2021-08-22T11:16:07ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-08-0181813910.1140/epjc/s10052-021-09475-0Multi-particle production in proton–nucleus collisions in the color glass condensatePedro Agostini0Tolga Altinoluk1Néstor Armesto2Instituto Galego de Física de Altas Enerxías IGFAE, Universidade de Santiago de CompostelaNational Centre for Nuclear ResearchInstituto Galego de Física de Altas Enerxías IGFAE, Universidade de Santiago de CompostelaAbstract We compute multi-gluon production in the Color Glass Condensate approach in dilute-dense collisions, $$\hbox {p}A$$ p A , extending previous calculations up to four gluons. We include the contributions that are leading in the overlap area of the collision but keep all orders in the expansion in the number of colors. We develop a diagrammatic technique to write the numerous color contractions and exploit the symmetries to group the diagrams and simplify the expressions. To proceed further, we use the McLerran–Venugopalan and Golec–Biernat–Wüsthoff models for the projectile and target averages, respectively. We use a form of the Lipatov vertices that leads to the Wigner function approach for the projectile previously employed, that we generalise to take into account quantum correlations in the projectile wave function. We provide analytic expressions for integrated and differential two gluon cumulants and show a smooth dependence on the parameters defining the projectile and target Wigner function and dipole, respectively. For four gluon correlations we find that the second order four particle cumulant is negative, so a sensible second Fourier azimuthal coefficient can be defined. The effect of correlations in the projectile on this result results qualitatively and quantitatively large.https://doi.org/10.1140/epjc/s10052-021-09475-0
collection DOAJ
language English
format Article
sources DOAJ
author Pedro Agostini
Tolga Altinoluk
Néstor Armesto
spellingShingle Pedro Agostini
Tolga Altinoluk
Néstor Armesto
Multi-particle production in proton–nucleus collisions in the color glass condensate
European Physical Journal C: Particles and Fields
author_facet Pedro Agostini
Tolga Altinoluk
Néstor Armesto
author_sort Pedro Agostini
title Multi-particle production in proton–nucleus collisions in the color glass condensate
title_short Multi-particle production in proton–nucleus collisions in the color glass condensate
title_full Multi-particle production in proton–nucleus collisions in the color glass condensate
title_fullStr Multi-particle production in proton–nucleus collisions in the color glass condensate
title_full_unstemmed Multi-particle production in proton–nucleus collisions in the color glass condensate
title_sort multi-particle production in proton–nucleus collisions in the color glass condensate
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2021-08-01
description Abstract We compute multi-gluon production in the Color Glass Condensate approach in dilute-dense collisions, $$\hbox {p}A$$ p A , extending previous calculations up to four gluons. We include the contributions that are leading in the overlap area of the collision but keep all orders in the expansion in the number of colors. We develop a diagrammatic technique to write the numerous color contractions and exploit the symmetries to group the diagrams and simplify the expressions. To proceed further, we use the McLerran–Venugopalan and Golec–Biernat–Wüsthoff models for the projectile and target averages, respectively. We use a form of the Lipatov vertices that leads to the Wigner function approach for the projectile previously employed, that we generalise to take into account quantum correlations in the projectile wave function. We provide analytic expressions for integrated and differential two gluon cumulants and show a smooth dependence on the parameters defining the projectile and target Wigner function and dipole, respectively. For four gluon correlations we find that the second order four particle cumulant is negative, so a sensible second Fourier azimuthal coefficient can be defined. The effect of correlations in the projectile on this result results qualitatively and quantitatively large.
url https://doi.org/10.1140/epjc/s10052-021-09475-0
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AT tolgaaltinoluk multiparticleproductioninprotonnucleuscollisionsinthecolorglasscondensate
AT nestorarmesto multiparticleproductioninprotonnucleuscollisionsinthecolorglasscondensate
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