Quantum Unitary and Pseudounitary Groups and Generalized Hadron Mass Relations

1995 ◽  
pp. 109-123 ◽  
Author(s):  
A. M. Gavrilik
Keyword(s):  
2019 ◽  
Vol 2019 ◽  
pp. 1-11 ◽  
Author(s):  
Guruprasad Kadam ◽  
Swapnali Pawar

We study the equation of state (EoS) of hot and dense hadron gas by incorporating the excluded volume corrections into the ideal hadron resonance gas (HRG) model. The total hadron mass spectrum of the model is the sum of the discrete mass spectrum consisting of all the experimentally known hadrons and the exponentially rising continuous Hagedorn states. We confront the EoS of the model with lattice quantum chromodynamics (LQCD) results at finite baryon chemical potential. We find that this modified HRG model reproduces the LQCD results up to T=160 MeV at zero as well as finite baryon chemical potential. We further estimate the shear viscosity within the ambit of this model in the context of heavy-ion collision experiments.


1987 ◽  
Vol 190 (1-2) ◽  
pp. 147-150 ◽  
Author(s):  
O. Haan ◽  
E. Schnepf ◽  
E. Laermann ◽  
K.H. Mütter ◽  
K. Schilling ◽  
...  
Keyword(s):  

2002 ◽  
Vol 109 (1) ◽  
pp. 50-54 ◽  
Author(s):  
S.V. Wright ◽  
D.B. Leinweber ◽  
A.W. Thomas ◽  
K. Tsushima
Keyword(s):  

1985 ◽  
Vol 162 (4-6) ◽  
pp. 354-356 ◽  
Author(s):  
K.C. Bowler ◽  
D.L. Chalmers ◽  
A. Kenway ◽  
R.D. Kenway ◽  
G.S. Pawley ◽  
...  
Keyword(s):  

Universe ◽  
2019 ◽  
Vol 5 (5) ◽  
pp. 122 ◽  
Author(s):  
Keming Shen ◽  
Gergely Gábor Barnaföldi ◽  
Tamás Sándor Biró

We investigate how the non-extensive approach works in high-energy physics. Transverse momentum ( p T ) spectra of several hadrons are fitted by various non-extensive momentum distributions and by the Boltzmann–Gibbs statistics. It is shown that some non-extensive distributions can be transferred one into another. We find explicit hadron mass and center-of-mass energy scaling both in the temperature and in the non-extensive parameter, q, in proton–proton and heavy-ion collisions. We find that the temperature depends linearly, but the Tsallis q follows a logarithmic dependence on the collision energy in proton–proton collisions. In the nucleus–nucleus collisions, on the other hand, T and q correlate linearly, as was predicted in our previous work.


1970 ◽  
Vol 68 (4) ◽  
pp. 605-611
Author(s):  
L. Goodman

1975 ◽  
Vol 12 (9) ◽  
pp. 2756-2760 ◽  
Author(s):  
A. W. Hendry ◽  
D. B. Lichtenberg

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