Microscopic foundations of Dirac phenomenology

1985 ◽  
Vol 31 (1) ◽  
pp. 63-68 ◽  
Author(s):  
L. S. Celenza ◽  
A. Harindranath ◽  
C. M. Shakin
Keyword(s):  
1990 ◽  
Vol 51 (C6) ◽  
pp. C6-111-C6-123
Author(s):  
J. A. TJON
Keyword(s):  

1983 ◽  
Author(s):  
B. C. Clark ◽  
S. Hama ◽  
R. L. Mercer

1995 ◽  
Vol 108 (9) ◽  
pp. 1103-1113
Author(s):  
M. A. Suhail ◽  
W. Haider ◽  
I. Ahmad

1994 ◽  
Vol 580 (3) ◽  
pp. 419-428 ◽  
Author(s):  
E.D. Cooper ◽  
B.K. Jennings ◽  
J. Mareš

1981 ◽  
Vol 23 (6) ◽  
pp. 2606-2615 ◽  
Author(s):  
M. R. Anastasio ◽  
L. S. Celenza ◽  
C. M. Shakin

2019 ◽  
Vol 18 ◽  
pp. 63
Author(s):  
T. Gaitanos ◽  
M. Kaskulov

The Lagrangian of Relativistic Hadrodynamics (RHD) is extended by introducing non-linear derivative (NLD) operators into the interactions between the nucleon with the meson elds. As the novel feature of the NLD model, the nucleon selfenergy depends on both, on energy and density. Our approach contains a single cut-o parameter, which determines the density dependence of the nuclear equation of state (EoS) and the energy dependence of the nucleon-nucleus optical potential. The NLD formalism is compatible with results from microscopic nuclear matter calculations as well as with Dirac phenomenology.


1995 ◽  
Vol 594 (3) ◽  
pp. 311-324 ◽  
Author(s):  
J. Mareš ◽  
E. Friedman ◽  
A. Gal ◽  
B.K. Jenning
Keyword(s):  

Author(s):  
S. Marcos ◽  
R. Niembro ◽  
M. López-Quelle ◽  
L. N. Savushkin ◽  
P. Bernardos

1994 ◽  
Vol 242 (4-6) ◽  
pp. 233-251 ◽  
Author(s):  
L. Zamick ◽  
D.C. Zheng

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