Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++
Abstract Recent experimental observations of the charged hadron properties in $$U+U$$ U+U collisions at 193 GeV contradict many of the theoretical models of particle production including two-component Monte Carlo Glauber model. The experimental results show a small correlation between the charged ha...
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doaj-743f1436f44443fab3d794d6d5c58efc2020-11-25T01:05:48ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-05-0178511310.1140/epjc/s10052-018-5908-8Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++Arpit Singh0P. K. Srivastava1O. S. K. Chaturvedi2S. Ahmad3B. K. Singh4Department of Physics, Institute of Science, Banaras Hindu UniversityDepartment of Physics, Indian Institute of Technology RoparDepartment of Physics, Institute of Science, Banaras Hindu UniversityDepartment of Physics, Aligarh Muslim UniversityDepartment of Physics, Institute of Science, Banaras Hindu UniversityAbstract Recent experimental observations of the charged hadron properties in $$U+U$$ U+U collisions at 193 GeV contradict many of the theoretical models of particle production including two-component Monte Carlo Glauber model. The experimental results show a small correlation between the charged hadron properties and the initial geometrical configurations (e.g. body–body, tip–tip etc.) of $$U+U$$ U+U collisions. In this article, we have modified the Monte Carlo HYDJET++ model to study the charged hadron production in $$U+U$$ U+U collisions at 193 GeV center-of-mass energy in tip–tip and body–body initial configurations. We have modified the hard as well as soft production processes to make this model suitable for $$U+U$$ U+U collisions. We have calculated the pseudorapidity distribution, transverse momentum distribution and elliptic flow distribution of charged hadrons with different control parameters in various geometrical configurations possible for $$U+U$$ U+U collision. We find that HYDJET++ model supports a small correlation between the various properties of charged hadrons and the initial geometrical configurations of $$U+U$$ U+U collision. Further, the results obtained in modified HYDJET++ model regarding $$dn_{ch}/d\eta $$ dnch/dη and elliptic flow ($$v_{2}$$ v2 ) suitably matches with the experimental data of $$U+U$$ U+U collisions in minimum bias configuration.http://link.springer.com/article/10.1140/epjc/s10052-018-5908-8 |
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DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Arpit Singh P. K. Srivastava O. S. K. Chaturvedi S. Ahmad B. K. Singh |
spellingShingle |
Arpit Singh P. K. Srivastava O. S. K. Chaturvedi S. Ahmad B. K. Singh Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++ European Physical Journal C: Particles and Fields |
author_facet |
Arpit Singh P. K. Srivastava O. S. K. Chaturvedi S. Ahmad B. K. Singh |
author_sort |
Arpit Singh |
title |
Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++ |
title_short |
Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++ |
title_full |
Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++ |
title_fullStr |
Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++ |
title_full_unstemmed |
Transverse momentum distribution and elliptic flow of charged hadrons in $$U+U$$ U+U collisions at $$\sqrt{s_{NN}}=193$$ sNN=193 GeV using HYDJET++ |
title_sort |
transverse momentum distribution and elliptic flow of charged hadrons in $$u+u$$ u+u collisions at $$\sqrt{s_{nn}}=193$$ snn=193 gev using hydjet++ |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2018-05-01 |
description |
Abstract Recent experimental observations of the charged hadron properties in $$U+U$$ U+U collisions at 193 GeV contradict many of the theoretical models of particle production including two-component Monte Carlo Glauber model. The experimental results show a small correlation between the charged hadron properties and the initial geometrical configurations (e.g. body–body, tip–tip etc.) of $$U+U$$ U+U collisions. In this article, we have modified the Monte Carlo HYDJET++ model to study the charged hadron production in $$U+U$$ U+U collisions at 193 GeV center-of-mass energy in tip–tip and body–body initial configurations. We have modified the hard as well as soft production processes to make this model suitable for $$U+U$$ U+U collisions. We have calculated the pseudorapidity distribution, transverse momentum distribution and elliptic flow distribution of charged hadrons with different control parameters in various geometrical configurations possible for $$U+U$$ U+U collision. We find that HYDJET++ model supports a small correlation between the various properties of charged hadrons and the initial geometrical configurations of $$U+U$$ U+U collision. Further, the results obtained in modified HYDJET++ model regarding $$dn_{ch}/d\eta $$ dnch/dη and elliptic flow ($$v_{2}$$ v2 ) suitably matches with the experimental data of $$U+U$$ U+U collisions in minimum bias configuration. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-018-5908-8 |
work_keys_str_mv |
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