Decomposition of harmonic and jet contributions to particle-pair correlations at ultrarelativistic energies

2005 ◽  
Vol 72 (1) ◽  
Author(s):  
N. N. Ajitanand ◽  
J. M. Alexander ◽  
P. Chung ◽  
W. G. Holzmann ◽  
M. Issah ◽  
...  
1991 ◽  
Vol 44 (3) ◽  
pp. 1091-1095 ◽  
Author(s):  
S. Wang ◽  
Y. Z. Jiang ◽  
Y. M. Liu ◽  
D. Keane ◽  
D. Beavis ◽  
...  

Symmetry ◽  
2021 ◽  
Vol 13 (8) ◽  
pp. 1405
Author(s):  
Feng Pan ◽  
Yingwen He ◽  
Lianrong Dai ◽  
Chong Qi ◽  
Jerry P. Draayer

A diagonalization scheme for the shell model mean-field plus isovector pairing Hamiltonian in the O(5) tensor product basis of the quasi-spin SUΛ(2) ⊗ SUI(2) chain is proposed. The advantage of the diagonalization scheme lies in the fact that not only can the isospin-conserved, charge-independent isovector pairing interaction be analyzed, but also the isospin symmetry breaking cases. More importantly, the number operator of the np-pairs can be realized in this neutron and proton quasi-spin basis, with which the np-pair occupation number and its fluctuation at the J = 0+ ground state of the model can be evaluated. As examples of the application, binding energies and low-lying J = 0+ excited states of the even–even and odd–odd N∼Z ds-shell nuclei are fit in the model with the charge-independent approximation, from which the neutron–proton pairing contribution to the binding energy in the ds-shell nuclei is estimated. It is observed that the decrease in the double binding-energy difference for the odd–odd nuclei is mainly due to the symmetry energy and Wigner energy contribution to the binding energy that alter the pairing staggering patten. The np-pair amplitudes in the np-pair stripping or picking-up process of these N = Z nuclei are also calculated.


2004 ◽  
Vol 41 (2) ◽  
pp. 207-212 ◽  
Author(s):  
T. Mehaddene ◽  
J. M. Sanchez ◽  
R. Caudron ◽  
M. Zemirli ◽  
V. Pierron-Bohnes

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