Time evolution of Mach-like structure in a partonic transport model
| dc.creator | Ma, G. L. | |
| dc.creator | Zhang, S. | |
| dc.creator | Ma, Y. G. | |
| dc.creator | Cai, X. Z. | |
| dc.creator | Chen, J. H. | |
| dc.creator | He, Z. J. | |
| dc.creator | Huang, H. Z. | |
| dc.creator | Long, J. L. | |
| dc.creator | Shen, W. Q. | |
| dc.creator | Shi, X. H. | |
| dc.creator | Zhong, C. | |
| dc.creator | Zuo, J. X. | |
| dc.date | 2006-10-24 | |
| dc.date.accessioned | 2026-07-07T07:29:49Z | |
| dc.date.available | 2026-07-07T07:29:49Z | |
| dc.description | The time evolution of Mach-like structure (the splitting of the away side peak in di-hadron $Δϕ$ correlation) is presented in the framework of a dynamical partonic transport model. With the increasing of the lifetime of partonic matter, Mach-like structure can be produced and developed by strong parton cascade process. Not only the splitting parameter but also the number of associated hadrons ($N_{h}^{assoc}$) increases with the lifetime of partonic matter and partonic interaction cross section. Both the explosion of $N_{h}^{assoc}$ following the formation of Mach-like structure and the corresponding results of three-particle correlation support that a partonic Mach-like shock wave can be formed by strong parton cascade mechanism. Therefore, the studies about Mach-like structure may give us some critical information, such as the lifetime of partonic matter and hadronization time. | |
| dc.description | 4 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/nucl-th/0610088 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/0610088 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/118258 | |
| dc.subject | Nuclear Theory | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | Nuclear Experiment | |
| dc.title | Time evolution of Mach-like structure in a partonic transport model | |
| dc.type | text |