In the present articles an attempt has been made for the determination of multiplicity fluctuations of the secondary charged particles produced in relativistic heavy ion collisions with the help of the Ginzburg-Landau (G-L) approach to find the first-order phase transition (QGP to hadron phase state). This study has been carried out for the experimental data along with the theoretical prediction of Ultra-relativistic Quantum Molecular Dynamics model (UrQMD) and Monte-Carlo (RanMC) simulation. The parameters of the theoretical model and the values of scaling exponent are found in good agreements.
| Published in | International Journal of High Energy Physics (Volume 4, Issue 5) |
| DOI | 10.11648/j.ijhep.20170405.12 |
| Page(s) | 58-64 |
| Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
| Copyright |
Copyright © The Author(s), 2017. Published by Science Publishing Group |
Multiplicity Distribution, Heavy Ion Collisions, Quark Gluon Plasma (QGP) Formation
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APA Style
Mohammad Ayaz Ahmad. (2017). Some Aspects of Simulations and Modeling in Relativistic Nuclear Collisions (Astro-Particle Physics). International Journal of High Energy Physics, 4(5), 58-64. https://doi.org/10.11648/j.ijhep.20170405.12
ACS Style
Mohammad Ayaz Ahmad. Some Aspects of Simulations and Modeling in Relativistic Nuclear Collisions (Astro-Particle Physics). Int. J. High Energy Phys. 2017, 4(5), 58-64. doi: 10.11648/j.ijhep.20170405.12
AMA Style
Mohammad Ayaz Ahmad. Some Aspects of Simulations and Modeling in Relativistic Nuclear Collisions (Astro-Particle Physics). Int J High Energy Phys. 2017;4(5):58-64. doi: 10.11648/j.ijhep.20170405.12
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Download@article{10.11648/j.ijhep.20170405.12,
author = {Mohammad Ayaz Ahmad},
title = {Some Aspects of Simulations and Modeling in Relativistic Nuclear Collisions (Astro-Particle Physics)},
journal = {International Journal of High Energy Physics},
volume = {4},
number = {5},
pages = {58-64},
doi = {10.11648/j.ijhep.20170405.12},
url = {https://doi.org/10.11648/j.ijhep.20170405.12},
eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijhep.20170405.12},
abstract = {In the present articles an attempt has been made for the determination of multiplicity fluctuations of the secondary charged particles produced in relativistic heavy ion collisions with the help of the Ginzburg-Landau (G-L) approach to find the first-order phase transition (QGP to hadron phase state). This study has been carried out for the experimental data along with the theoretical prediction of Ultra-relativistic Quantum Molecular Dynamics model (UrQMD) and Monte-Carlo (RanMC) simulation. The parameters of the theoretical model and the values of scaling exponent are found in good agreements.},
year = {2017}
}
TY - JOUR T1 - Some Aspects of Simulations and Modeling in Relativistic Nuclear Collisions (Astro-Particle Physics) AU - Mohammad Ayaz Ahmad Y1 - 2017/11/10 PY - 2017 N1 - https://doi.org/10.11648/j.ijhep.20170405.12 DO - 10.11648/j.ijhep.20170405.12 T2 - International Journal of High Energy Physics JF - International Journal of High Energy Physics JO - International Journal of High Energy Physics SP - 58 EP - 64 PB - Science Publishing Group SN - 2376-7448 UR - https://doi.org/10.11648/j.ijhep.20170405.12 AB - In the present articles an attempt has been made for the determination of multiplicity fluctuations of the secondary charged particles produced in relativistic heavy ion collisions with the help of the Ginzburg-Landau (G-L) approach to find the first-order phase transition (QGP to hadron phase state). This study has been carried out for the experimental data along with the theoretical prediction of Ultra-relativistic Quantum Molecular Dynamics model (UrQMD) and Monte-Carlo (RanMC) simulation. The parameters of the theoretical model and the values of scaling exponent are found in good agreements. VL - 4 IS - 5 ER -
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