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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...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2005
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.physletb.2005.08.131 http://cds.cern.ch/record/865487 |
_version_ | 1780907312686301184 |
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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 |