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Elliptic flow and incomplete equilibration at RHIC

We argue that RHIC data, in particular those on the anisotropic flow coefficients v_2 and v_4, suggest that the matter produced in the early stages of nucleus-nucleus collisions is incompletely thermalized. We interpret the parameter (1/S)(dN/dy), where S is the transverse area of the collision zone...

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Detalles Bibliográficos
Autores principales: Bhalerao, R S, Blaizot, J P, Borghini, N, Ollitrault, Jean Yves
Lenguaje:eng
Publicado: 2005
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2005.08.131
http://cds.cern.ch/record/865487
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author Bhalerao, R S
Blaizot, J P
Borghini, N
Ollitrault, Jean Yves
author_facet Bhalerao, R S
Blaizot, J P
Borghini, N
Ollitrault, Jean Yves
author_sort Bhalerao, R S
collection CERN
description We argue that RHIC data, in particular those on the anisotropic flow coefficients v_2 and v_4, suggest that the matter produced in the early stages of nucleus-nucleus collisions is incompletely thermalized. We interpret the parameter (1/S)(dN/dy), where S is the transverse area of the collision zone and dN/dy the multiplicity density, as an indicator of the number of collisions per particle at the time when elliptic flow is established, and hence as a measure of the degree of equilibration. This number serves as a control parameter which can be varied experimentally by changing the system size, the centrality or the beam energy. We provide predictions for Cu-Cu collisions at RHIC as well as for Pb-Pb collisions at the LHC.
id cern-865487
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2005
record_format invenio
spelling cern-8654872019-09-30T06:29:59Zdoi:10.1016/j.physletb.2005.08.131http://cds.cern.ch/record/865487engBhalerao, R SBlaizot, J PBorghini, NOllitrault, Jean YvesElliptic flow and incomplete equilibration at RHICNuclear Physics - TheoryWe argue that RHIC data, in particular those on the anisotropic flow coefficients v_2 and v_4, suggest that the matter produced in the early stages of nucleus-nucleus collisions is incompletely thermalized. We interpret the parameter (1/S)(dN/dy), where S is the transverse area of the collision zone and dN/dy the multiplicity density, as an indicator of the number of collisions per particle at the time when elliptic flow is established, and hence as a measure of the degree of equilibration. This number serves as a control parameter which can be varied experimentally by changing the system size, the centrality or the beam energy. We provide predictions for Cu-Cu collisions at RHIC as well as for Pb-Pb collisions at the LHC.nucl-th/0508009CERN-PH-TH-2005-143ECT-2005-06SACLAY-SPHT-T-2005-126TIFR-TH-2005-30oai:cds.cern.ch:8654872005-08-03
spellingShingle Nuclear Physics - Theory
Bhalerao, R S
Blaizot, J P
Borghini, N
Ollitrault, Jean Yves
Elliptic flow and incomplete equilibration at RHIC
title Elliptic flow and incomplete equilibration at RHIC
title_full Elliptic flow and incomplete equilibration at RHIC
title_fullStr Elliptic flow and incomplete equilibration at RHIC
title_full_unstemmed Elliptic flow and incomplete equilibration at RHIC
title_short Elliptic flow and incomplete equilibration at RHIC
title_sort elliptic flow and incomplete equilibration at rhic
topic Nuclear Physics - Theory
url https://dx.doi.org/10.1016/j.physletb.2005.08.131
http://cds.cern.ch/record/865487
work_keys_str_mv AT bhaleraors ellipticflowandincompleteequilibrationatrhic
AT blaizotjp ellipticflowandincompleteequilibrationatrhic
AT borghinin ellipticflowandincompleteequilibrationatrhic
AT ollitraultjeanyves ellipticflowandincompleteequilibrationatrhic