Factorization of fragment-production cross sections in relativistic heavy-ion collisions

1983 ◽  
Vol 28 (4) ◽  
pp. 1602-1613 ◽  
Author(s):  
D. L. Olson ◽  
B. L. Berman ◽  
D. E. Greiner ◽  
H. H. Heckman ◽  
P. J. Lindstrom ◽  
...  
Keyword(s):  
Cross Sections ◽  
Heavy Ion Collisions ◽  
Production Cross ◽  
Heavy Ion ◽  
Relativistic Heavy Ion Collisions ◽  
Ion Collisions ◽  
Fragment Production

scholarly journals Review of Charmonium and Bottomonium Quark State Production via Relativistic Heavy Ion Collisions

Universe ◽  
2020 ◽  
Vol 6 (1) ◽  
pp. 13
Author(s):  
Leonard S. Kisslinger
Keyword(s):  
Heavy Quark ◽  
Cross Sections ◽  
Heavy Ion Collisions ◽  
Production Cross ◽  
Charm Quark ◽  
Heavy Ion ◽  
Gluon Plasma ◽  
Relativistic Heavy Ion Collisions ◽  
Ion Collisions ◽  
Meson States

This is a review of the production of heavy quark states via relativistic heavy ion collisions in RHIC. The heavy quarks here are c, charm quark, and b, bottom quark. The states are charmonium meson states Ψ ( n S ) , with n = 1,2 and upsilon meson states Υ ( m S ) , with m = 1,2,3. Quantum Chromodynamics (QCD) sum rules were used to derive the result that the Ψ ( 2 S ) and Υ ( 3 S ) are mixed hybrid states, which increase their production cross sections. We also review the Ψ ( n S ) and Υ ( m S ) production cross sections via Cu-Cu and Au-Au collisions, which are very important for this review of the production of heavy quark states in RHIC. The possible detection of the Quark Gluon Plasma (QGP) is also reviewed.

Cross sections for photons produced in the stopping phase in relativistic heavy-ion collisions

1989 ◽  
Vol 504 (4) ◽  
pp. 864-874 ◽  
Author(s):  
Joachim Thiel ◽  
Thomas Lippert ◽  
Norbert Grün ◽  
Werner Scheid
Keyword(s):  
Cross Sections ◽  
Heavy Ion Collisions ◽  
Heavy Ion ◽  
Relativistic Heavy Ion Collisions ◽  
Ion Collisions

scholarly journals An Experimental Review on Elliptic Flow of Strange and Multistrange Hadrons in Relativistic Heavy Ion Collisions

2016 ◽  
Vol 2016 ◽  
pp. 1-9 ◽  
Author(s):  
Shusu Shi
Keyword(s):  
Large Hadron Collider ◽  
Cross Sections ◽  
Heavy Ion Collisions ◽  
Hadron Collider ◽  
Elliptic Flow ◽  
Heavy Ion ◽  
Relativistic Heavy Ion Collisions ◽  
Relativistic Heavy Ion Collider ◽  
Flow Measurements ◽  
Ion Collisions

Strange hadrons, especially multistrange hadrons, are good probes for the early partonic stage of heavy ion collisions due to their small hadronic cross sections. In this paper, I give a brief review on the elliptic flow measurements of strange and multistrange hadrons in relativistic heavy ion collisions at Relativistic Heavy Ion Collider (RHIC) and Large Hadron Collider (LHC).

Fragmentation cross sections and search for nuclear fragments with fractional charge in relativistic heavy ion collisions

1993 ◽  
Vol 1 (4) ◽  
pp. 369-376 ◽  
Author(s):  
S. Cecchini ◽  
H. Dekhissi ◽  
G. Giacomelli ◽  
G. Mandrioli ◽  
A.R. Margiotta ◽  
...  
Keyword(s):  
Cross Sections ◽  
Heavy Ion Collisions ◽  
Heavy Ion ◽  
Relativistic Heavy Ion Collisions ◽  
Fractional Charge ◽  
Ion Collisions

FRAGMENTATION CROSS SECTIONS IN HEAVY ION COLLISIONS

2008 ◽  
Vol 17 (09) ◽  
pp. 1927-1936
Author(s):  
BAO-AN BIAN ◽  
FENG-SHOU ZHANG ◽  
HONG-YU ZHOU
Keyword(s):  
Cross Sections ◽  
Langevin Equation ◽  
Heavy Ion Collisions ◽  
Production Cross ◽  
Heavy Ion ◽  
Ion Collisions ◽  
Target Mass

The fragment cross sections are calculated for reactions of Ne collisions with C , Al , Cu , Sn , Ta , and Pb targets at 600 Mev/nucleon using the the isospin-dependent Boltzmann-Langevin equation. We found that the production cross sections for fragments Z = 2 to 9 are qualitatively reproduced by the present calculations except for C target. In order to understand the effects of heavy ion interaction with biomolecules well, we calculate the fragmentation cross sections for reactions of 12 C + 2 H , 12 C , 14 N , 16 O at beam energies from 50 to 100 MeV/nucleon. It is found that fragment species increase approximately with increasing target mass. The obvious increment of the fragment cross sections for heavier targets at the beam energies from 50 to 80 MeV/nucleon are shown.

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