Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
8184311 | Nuclear Physics A | 2013 | 4 Pages |
Abstract
A baryon anomaly - an increased baryon-to-meson production ratio at intermediate pT in heavyion 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.
Related Topics
Physical Sciences and Engineering
Physics and Astronomy
Nuclear and High Energy Physics
Authors
Eugene M. Levin, Gustaw Matulewicz, Mikhail G. Ryskin, Karel Å afaÅÃk,