$$Z_b(10610)$$ Zb(10610) in a hadronic medium

Abstract In this work we investigate the $$Z_b (10610)$$ Zb(10610) (called simply $$Z_b$$ Zb ) abundance in the hot hadron gas produced in heavy ion collisions after the quark–gluon plasma phase. We use effective Lagrangians to calculate the thermally averaged cross sections of $$Z_b $$ Zb productio...

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Main Authors: L. M. Abreu, F. S. Navarra, M. Nielsen, A. L. Vasconcellos
Format: Article
Language:English
Published: SpringerOpen 2018-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-018-6182-5
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author L. M. Abreu
F. S. Navarra
M. Nielsen
A. L. Vasconcellos
author_facet L. M. Abreu
F. S. Navarra
M. Nielsen
A. L. Vasconcellos
author_sort L. M. Abreu
collection DOAJ
description Abstract In this work we investigate the $$Z_b (10610)$$ Zb(10610) (called simply $$Z_b$$ Zb ) abundance in the hot hadron gas produced in heavy ion collisions after the quark–gluon plasma phase. We use effective Lagrangians to calculate the thermally averaged cross sections of $$Z_b $$ Zb production in processes such as $$B^{(*)} + \bar{B}^{(*)} \rightarrow \pi + Z_b (10610)$$ B(∗)+B¯(∗)→π+Zb(10610) and also of its absorption in the corresponding inverse processes. We then solve the rate equation to follow the time evolution of the $$Z_b$$ Zb multiplicity. We find that, if we neglect the $$Z_b$$ Zb decay, the number of $$Z_b$$ Zb ’s produced at the end of the quark–gluon plasma phase remains almost constant during the hadron phase. The introduction of the decay in the rate equation leads to a suppression in the final yield by a factor two.
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spelling doaj.art-774557c0b99042b3b896fc14289d18c12022-12-21T18:25:24ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-09-017891810.1140/epjc/s10052-018-6182-5$$Z_b(10610)$$ Zb(10610) in a hadronic mediumL. M. Abreu0F. S. Navarra1M. Nielsen2A. L. Vasconcellos3Instituto de Física, Universidade Federal da BahiaInstituto de Física, Universidade de São PauloInstituto de Física, Universidade de São PauloInstituto de Física, Universidade Federal da BahiaAbstract In this work we investigate the $$Z_b (10610)$$ Zb(10610) (called simply $$Z_b$$ Zb ) abundance in the hot hadron gas produced in heavy ion collisions after the quark–gluon plasma phase. We use effective Lagrangians to calculate the thermally averaged cross sections of $$Z_b $$ Zb production in processes such as $$B^{(*)} + \bar{B}^{(*)} \rightarrow \pi + Z_b (10610)$$ B(∗)+B¯(∗)→π+Zb(10610) and also of its absorption in the corresponding inverse processes. We then solve the rate equation to follow the time evolution of the $$Z_b$$ Zb multiplicity. We find that, if we neglect the $$Z_b$$ Zb decay, the number of $$Z_b$$ Zb ’s produced at the end of the quark–gluon plasma phase remains almost constant during the hadron phase. The introduction of the decay in the rate equation leads to a suppression in the final yield by a factor two.http://link.springer.com/article/10.1140/epjc/s10052-018-6182-5
spellingShingle L. M. Abreu
F. S. Navarra
M. Nielsen
A. L. Vasconcellos
$$Z_b(10610)$$ Zb(10610) in a hadronic medium
European Physical Journal C: Particles and Fields
title $$Z_b(10610)$$ Zb(10610) in a hadronic medium
title_full $$Z_b(10610)$$ Zb(10610) in a hadronic medium
title_fullStr $$Z_b(10610)$$ Zb(10610) in a hadronic medium
title_full_unstemmed $$Z_b(10610)$$ Zb(10610) in a hadronic medium
title_short $$Z_b(10610)$$ Zb(10610) in a hadronic medium
title_sort z b 10610 zb 10610 in a hadronic medium
url http://link.springer.com/article/10.1140/epjc/s10052-018-6182-5
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AT fsnavarra zb10610zb10610inahadronicmedium
AT mnielsen zb10610zb10610inahadronicmedium
AT alvasconcellos zb10610zb10610inahadronicmedium