Baryon Anomaly in Heavy-Ion Collisions and Colour Correlations in QGP

被引:1
作者
Levin, Eugene M. [1 ,2 ,3 ]
Matulewicz, Gustaw [4 ]
Ryskin, Mikhail G. [5 ]
Safaik, Karel [4 ]
机构
[1] Tel Aviv Univ, Sch Phys & Astron, IL-69978 Tel Aviv, Israel
[2] Univ Tecn Federico Santa Maria, Valparaiso, Chile
[3] Ctr Cientif Tecnol Valparalso, Valparaiso, Chile
[4] CERN, CH-1211 Geneva 23, Switzerland
[5] NRC Kurchatov Inst, Petersburg Nucl Phys Inst, St Petersburg, Russia
关键词
QUARK-MODEL; MULTIPARTICLE;
D O I
10.1016/j.nuclphysa.2013.02.040
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
A baryon anomaly - an increased baryon-to-meson production ratio at intermediate p(T) in heavy-ion collisions when compared to pp collisions - is observed at RHIC and the LHC. This effect is usually explained by recombination of constituent quarks during QGP hadronization, or as a consequence of a strong radial flow developed during the heavy-ion collision. In this contribution, an additional mechanism to favour baryon over meson production is proposed: when hadrons are formed in the recombination of nearby quarks and antiquarks, only colour-singlet combinations can be chosen. Hadron formation, in particular the probability to create baryons or mesons, depends on the distribution of colour charges among quarks. If the distribution is random - a reasonable assumption for Quark-Gluon Plasma (QGP) - the baryon-to-meson ratio is nearly twice higher than in the situation where quark colours are pre-arranged to obtain a white hadron in the combination of nearest quarks and antiquarks. The correlation of colour charges in the QGP also influences the distance over which recombination occurs. A study of the dependence of the baryon-to-meson ratio on the size of the colour correlation domain is presented.
引用
收藏
页码:425C / 428C
页数:4
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