Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamics

We compute single and double inclusive gluon distributions in classical Yang–Mills simulations of proton–lead collisions and extract the associated transverse momentum dependent Fourier harmonics v2(pT) and v3(pT). Gluons have a large v2 in the initial state, while odd harmonics such as v3 vanish id...

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Main Authors: Björn Schenke, Sören Schlichting, Raju Venugopalan
Format: Article
Language:English
Published: Elsevier 2015-07-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269315003883
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spelling doaj-516311dfa9d249cfa235c61ad0b91afd2020-11-24T21:04:06ZengElsevierPhysics Letters B0370-26931873-24452015-07-01747C768210.1016/j.physletb.2015.05.051Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamicsBjörn SchenkeSören SchlichtingRaju VenugopalanWe compute single and double inclusive gluon distributions in classical Yang–Mills simulations of proton–lead collisions and extract the associated transverse momentum dependent Fourier harmonics v2(pT) and v3(pT). Gluons have a large v2 in the initial state, while odd harmonics such as v3 vanish identically at the initial time τ=0+. By the time τ≲0.4 fm/c final state effects in the classical Yang–Mills evolution generate a non-zero v3 and only mildly modify the gluon v2. Unlike hydrodynamic flow, these momentum space anisotropies are uncorrelated with the global spatial anisotropy of the collision. A principal ingredient for the generation of v2 and v3 in this framework is the event-by-event breaking of rotational invariance in domains the size of the inverse of the saturation scale Qs. In contrast to our findings in p+Pb collisions Yang–Mills simulations of lead–lead collisions generate much smaller values of v2,3(pT) and additional collective flow effects are needed to explain experimental data. This is because the locally generated anisotropy due to the breaking of rotational invariance is depleted with the increase in the number of uncorrelated domains.http://www.sciencedirect.com/science/article/pii/S0370269315003883
collection DOAJ
language English
format Article
sources DOAJ
author Björn Schenke
Sören Schlichting
Raju Venugopalan
spellingShingle Björn Schenke
Sören Schlichting
Raju Venugopalan
Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamics
Physics Letters B
author_facet Björn Schenke
Sören Schlichting
Raju Venugopalan
author_sort Björn Schenke
title Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamics
title_short Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamics
title_full Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamics
title_fullStr Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamics
title_full_unstemmed Azimuthal anisotropies in p+Pb collisions from classical Yang–Mills dynamics
title_sort azimuthal anisotropies in p+pb collisions from classical yang–mills dynamics
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2015-07-01
description We compute single and double inclusive gluon distributions in classical Yang–Mills simulations of proton–lead collisions and extract the associated transverse momentum dependent Fourier harmonics v2(pT) and v3(pT). Gluons have a large v2 in the initial state, while odd harmonics such as v3 vanish identically at the initial time τ=0+. By the time τ≲0.4 fm/c final state effects in the classical Yang–Mills evolution generate a non-zero v3 and only mildly modify the gluon v2. Unlike hydrodynamic flow, these momentum space anisotropies are uncorrelated with the global spatial anisotropy of the collision. A principal ingredient for the generation of v2 and v3 in this framework is the event-by-event breaking of rotational invariance in domains the size of the inverse of the saturation scale Qs. In contrast to our findings in p+Pb collisions Yang–Mills simulations of lead–lead collisions generate much smaller values of v2,3(pT) and additional collective flow effects are needed to explain experimental data. This is because the locally generated anisotropy due to the breaking of rotational invariance is depleted with the increase in the number of uncorrelated domains.
url http://www.sciencedirect.com/science/article/pii/S0370269315003883
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AT sorenschlichting azimuthalanisotropiesinppbcollisionsfromclassicalyangmillsdynamics
AT rajuvenugopalan azimuthalanisotropiesinppbcollisionsfromclassicalyangmillsdynamics
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