Using the HIJING Model in Modeling Nucleus–Nucleus Interaction at Energies of Nucleon–Nucleon Collisions 5–15 GeV

2020 ◽  
Vol 84 (4) ◽  
pp. 446-450
Author(s):  
A. S. Galoyan ◽  
V. V. Uzhinsky
1979 ◽  
Vol 57 (11) ◽  
pp. 2026-2029 ◽  
Author(s):  
Dipak Ghosh ◽  
Sadhan Naha ◽  
Jaya Roy ◽  
Anuradha Bhattacharjee ◽  
Topen Roy

This paper presents a first investigation of the cluster production in nucleon – heavy nucleus collision in emulsion at cosmic ray energies (up to 1 TeV) following a model independent method proposed in a recent paper by Shivpuri and Gupta. It has been observed that the maximum charged pions constituting a cluster is three up to this energy and cluster characteristics are the same as in the case of nucleon–nucleon interaction in the same energy region.


1975 ◽  
Vol 11 (2) ◽  
pp. 437-449 ◽  
Author(s):  
L. S. Celenza ◽  
L. C. Liu ◽  
C. M. Shakin

Universe ◽  
2021 ◽  
Vol 7 (6) ◽  
pp. 203
Author(s):  
Peter Shternin ◽  
Isaac Vidaña

We consider transport properties of the hypernuclear matter in neutron star cores. In particular, we calculate the thermal conductivity, the shear viscosity, and the momentum transfer rates for npΣ−Λeμ composition of dense matter in β–equilibrium for baryon number densities in the range 0.1–1 fm−3. The calculations are based on baryon interactions treated within the framework of the non-relativistic Brueckner-Hartree-Fock theory. Bare nucleon-nucleon (NN) interactions are described by the Argonne v18 phenomenological potential supplemented with the Urbana IX three-nucleon force. Nucleon-hyperon (NY) and hyperon-hyperon (YY) interactions are based on the NSC97e and NSC97a models of the Nijmegen group. We find that the baryon contribution to transport coefficients is dominated by the neutron one as in the case of neutron star cores containing only nucleons. In particular, we find that neutrons dominate the total thermal conductivity over the whole range of densities explored and that, due to the onset of Σ− which leads to the deleptonization of the neutron star core, they dominate also the shear viscosity in the high density region, in contrast with the pure nucleonic case where the lepton contribution is always the dominant one.


1950 ◽  
Vol 5 (2) ◽  
pp. 318-318
Author(s):  
F. Fujimoto ◽  
S. Hayakawa ◽  
Y. Yamaguchi

1990 ◽  
Vol 05 (14) ◽  
pp. 1071-1080 ◽  
Author(s):  
S. W. HUANG ◽  
M. Z. FU ◽  
S. S. WU ◽  
S. D. YANG

The equation of state of the asymmetric nuclear matter is calculated with the Gogny D1 effective density-dependent nucleon-nucleon interaction and the Coulomb interaction in the framework of the finite-temperature HF method with the rearrangement term. The dependence of the thermodynamical properties such as the critical temperature of the liquid-gas phase transition, the chemical potential, the compression modulus and the entropy on the Coulomb interaction in nuclear matter is treated by using a shielded two-body Coulomb potential and this method has been found to be a reasonable and effective approach.


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