Incompressibility of Nuclear Matter from the Giant Monopole Resonance

1999 ◽  
Vol 82 (4) ◽  
pp. 691-694 ◽  
Author(s):  
D. H. Youngblood ◽  
H. L. Clark ◽  
Y.-W. Lui
1994 ◽  
Vol 569 (1-2) ◽  
pp. 303-312 ◽  
Author(s):  
S. Shlomo ◽  
D.H. Youngblood

1993 ◽  
Vol 47 (2) ◽  
pp. 529-536 ◽  
Author(s):  
S. Shlomo ◽  
D. H. Youngblood

2006 ◽  
Vol 15 (08) ◽  
pp. 1909-1923
Author(s):  
SHALOM SHLOMO ◽  
V. KIM AU

Bulk properties of nuclear matter associated with the equation of state, the nuclear matter incompressibility coefficient, Knm, in particular, are very important physical quantities required in the study of properties of nuclei, supernova collapse, neutron stars and heavy-ion collisions. Here we review the current status of Knm and the experimental and theoretical methods used to determine the value of Knm from the excitation cross-sections and the transition strength distributions of compression modes in nuclei, mainly the the isoscalar giant monopole resonance and the isoscalar giant dipole resonance.


1999 ◽  
Vol 649 (1-4) ◽  
pp. 49-56 ◽  
Author(s):  
D.H. Youngblood ◽  
H.L. Clark ◽  
Y.-W. Lui

2015 ◽  
Vol 30 (20) ◽  
pp. 1550097 ◽  
Author(s):  
S. K. Biswal ◽  
S. K. Singh ◽  
S. K. Patra

Within the framework of relativistic Thomas–Fermi (RTF) and relativistic extended Thomas–Fermi (RETF) approximations, we calculate the giant monopole resonance (GMR) excitation energies for Sn and related nuclei. A large number of nonlinear relativistic force parameters are used in these calculations. We find a parameter set is capable to reproduce the experimental monopole energy of Sn isotopes, when its nuclear matter compressibility lies within 210–230 MeV, however, it fails to reproduce the GMR energy of other nuclei. That means, simultaneously a parameter set cannot reproduce the GMR values of Sn and other nuclei.


1988 ◽  
Vol 38 (6) ◽  
pp. 2562-2572 ◽  
Author(s):  
M. M. Sharma ◽  
W. T. A. Borghols ◽  
S. Brandenburg ◽  
S. Crona ◽  
A. van der Woude ◽  
...  

1987 ◽  
Vol 48 (C2) ◽  
pp. C2-301-C2-304
Author(s):  
M. BALDO ◽  
G. GIANSIRACUSA ◽  
U. LOMBARDO

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