scholarly journals A novel method for determining the mean-field directly from the single particle matter density

2015 ◽  
Vol 633 ◽  
pp. 012028 ◽  
Author(s):  
S Shlomo ◽  
M R Anders ◽  
I Talmi
2006 ◽  
Vol 21 (31n33) ◽  
pp. 2475-2482
Author(s):  
SATORU SUGIMOTO

We study the effect of the tensor correlation using a mean-field-type model and a shell model. To treat the tensor correlation in a mean-field-type model, we introduce single-particle states with the parity and charge mixing considering the pseudoscalar and isovector characters of the pion, which mediates the tensor force. We study closed-shell and sub-closed-shell oxygen isotopes and find that a sizable attractive energy from the tensor force is obtained by introducing the parity and charge mixing. We also perform a shell model calculation up to two-particle–two-hole configurations. A large attraction energy is obtained for 16 O when we introduce single-particle wave functions with narrow widths.


2006 ◽  
Vol 20 (32) ◽  
pp. 5443-5462 ◽  
Author(s):  
TARUN KANTI GHOSH

We analytically study effects of density and phase fluctuations of quasi-one-dimensional degenerate atomic Bose gases in the mean-field as well as in the hard-core bosons regimes. We obtain the analytic expressions for dynamic structure factors in both the regimes. We also calculate single-particle density matrix and momentum distribution by taking care of the phase fluctuations upto fourth-order term, the density fluctuations as well as the non-condensate density in both the regimes. In the mean-field regime, there is a long-tail in the momentum distributions at large temperature, which can be used to identify the quasi-condensate from a pure condensate. The single-particle correlation functions of hard-core bosons is almost zero even at zero temperature due to the fermionization of the bosonic systems. Two-particle correlation function in the hard-core bosons regime shows many deep valleys at various relative separations. These valleys at various relative separations imply shell structure due to the Pauli blocking in real space.


2009 ◽  
Vol 73 (11) ◽  
pp. 1442-1445 ◽  
Author(s):  
O. V. Bespalova ◽  
I. N. Boboshin ◽  
V. V. Varlamov ◽  
B. S. Ishkhanov ◽  
E. A. Romanovskii ◽  
...  

2019 ◽  
Vol 66 (1) ◽  
pp. 82
Author(s):  
R. Gupta ◽  
S. Sunder Malik

We have presented the single particle spectrum for a particle in a mean field of isotropic harmonic oscillator with l.s  coupling based on our semiclassical approach. It has been seen that this spectrum, without l.s  coupling, exactly matches with the quantum mechanical one (without nuclear constraints). In this case, periodicity conditions give only pendulating orbits coinciding with l=0 axis, which fully support the observations reported by Bohr and Mottelson [28]. The orbits with l>0 are generated by reflecting the particle from the nuclear surface, instead of infinity, which is the usual nuclear constraint. The mean field strength is fixed by virial theorem. The resulting spectrum compares reasonably with the quantum spectrum for a particle enclosed in a perfectly reflecting walls. The variation of particle number with energy help us to identify the significant quantum numbers n and l in this semiclassical method. Finally, the l.s coupling splits each level and the splitting width of these level compares well with that of nuclear splitting. Thus the complete nuclear shell model (with magic numbers) is reproduced without any fitting parameter.


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