scholarly journals Thermalization of gluons at RHIC including gg ↔ ggg interactions in a parton cascade

2006 ◽  
Vol 774 ◽  
pp. 787-790 ◽  
Author(s):  
Z. Xu ◽  
C. Greiner
Keyword(s):  
Parton Cascade

PARTON RECOMBINATION IN CLASSICAL CASCADE

1990 ◽  
Vol 05 (28) ◽  
pp. 2377-2383 ◽  
Author(s):  
A. V. BATUNIN ◽  
O. P. YUSHCHENKO
Keyword(s):  
Explicit Form ◽  
Heavy Ion Collisions ◽  
Charged Particles ◽  
Heavy Ion ◽  
Considerable Decrease ◽  
High Energies ◽  
Ion Collisions ◽  
Parton Cascade ◽  
Energy Formula ◽  
The Mean

An equation for parton multiplicity in cascade with the recombination 1 → 2 ⊕ 2 → 1 is derived from a Kolmogorov-Chapman equation and solved. An evolution parameter τ of the cascade depends on the c.m. energy [Formula: see text]; an explicit form of the dependence is obtained from the condition that the mean multiplicity of charged particles in pp, [Formula: see text] collisions be reproduced. A considerable decrease in the mean multiplicity in heavy-ion collisions per pair of the colliding nucleons at high energies is predicted and compared to the parton cascade with no recombination.

scholarly journals Elliptic flow from a parton cascade

1999 ◽  
Vol 455 (1-4) ◽  
pp. 45-48 ◽  
Author(s):  
Bin Zhang ◽  
Miklos Gyulassy ◽  
Che Ming Ko
Keyword(s):  
Elliptic Flow ◽  
Parton Cascade

Equilibration of two power-law tailed distributions in a parton cascade model

2008 ◽  
Vol 372 (8) ◽  
pp. 1174-1179 ◽  
Author(s):  
Tamás S. Bíró ◽  
Gábor Purcsel
Keyword(s):  
Power Law ◽  
Cascade Model ◽  
Parton Cascade

“TEMPERATURE” FLUCTUATION AND HEAT CAPACITIES OF QUARKS AND π MESON

2007 ◽  
Vol 16 (07n08) ◽  
pp. 1912-1916
Author(s):  
X. H. SHI ◽  
G. L. MA ◽  
Y. G. MA ◽  
X. Z. CAI ◽  
J. H. CHEN
Keyword(s):  
Heat Capacity ◽  
Specific Heat ◽  
Impact Parameter ◽  
Specific Heat Capacity ◽  
Temperature Fluctuation ◽  
Temperature Fluctuations ◽  
Heat Capacities ◽  
Transverse Mass ◽  
Parton Cascade ◽  
Specific Heat Capacities

Specific heat capacities of π meson and different quarks after parton cascade AMPT model in Au + Au collisions at [Formula: see text] have been tentatively extracted from the event-by-event temperature fluctuations in the region of low transverse mass. The specific heat capacity of π meson shows a slight dropping trend with increasing impact parameter. The specific heat capacities of different quarks increase with the mass of quark, and the sum of up and down quark's specific heat capacities was found to be approximately equal to that of π meson.

scholarly journals Calculation of shear viscosity using Green-Kubo relations within a parton cascade

2011 ◽  
Vol 84 (5) ◽  
Author(s):  
C. Wesp ◽  
A. El ◽  
F. Reining ◽  
Z. Xu ◽  
I. Bouras ◽  
...  
Keyword(s):  
Shear Viscosity ◽  
Parton Cascade

scholarly journals APACIC++ 2.0. A PArton Cascade In C++

2006 ◽  
Vol 174 (11) ◽  
pp. 876-902 ◽  
Author(s):  
F. Krauss ◽  
A. Schälicke ◽  
G. Soff
Keyword(s):  
Parton Cascade

scholarly journals Universal quark to gluon ratio in medium-induced parton cascade

2018 ◽  
Vol 2018 (9) ◽  
Author(s):  
Yacine Mehtar-Tani ◽  
Soeren Schlichting
Keyword(s):  
Parton Cascade

scholarly journals The parton cascade BAMPS with the improved Gunion-Bertsch matrix element

2014 ◽  
Author(s):  
Carsten Greiner ◽  
Florian Senzel ◽  
Oliver Fochler ◽  
Jan Uphoff ◽  
Christian WESP ◽  
...  
Keyword(s):  
Matrix Element ◽  
Parton Cascade

scholarly journals Further developments of a multi-phase transport model for relativistic nuclear collisions

2021 ◽  
Vol 32 (10) ◽  
Author(s):  
Zi-Wei Lin ◽  
Liang Zheng
Keyword(s):  
Transport Model ◽  
Dense Matter ◽  
Nuclear Collisions ◽  
Future Developments ◽  
Parton Cascade ◽  
Large Systems ◽  
Relativistic Nuclear Collisions ◽  
Main Components ◽  
Multi Phase ◽  
Phase Transport

AbstractA multi-phase transport (AMPT) model was constructed as a self-contained kinetic theory-based description of relativistic nuclear collisions as it contains four main components: the fluctuating initial condition, a parton cascade, hadronization, and a hadron cascade. Here, we review the main developments after the first public release of the AMPT source code in 2004 and the corresponding publication that described the physics details of the model at that time. We also discuss possible directions for future developments of the AMPT model to better study the properties of the dense matter created in relativistic collisions of small or large systems.

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