Energy dependence of the mean-field potential for neutron scattering from190,192Os and194,196Pt

1988 ◽  
Vol 37 (4) ◽  
pp. 1787-1790 ◽  
Author(s):  
S. E. Hicks ◽  
M. T. McEllistrem
Keyword(s):  
Neutron Scattering ◽  
Energy Dependence ◽  
Mean Field ◽  
Field Potential ◽  
The Mean ◽  
Mean Field Potential

Restudy of surface tension of QGP with one-loop correction in the mean-field potential

2014 ◽  
Vol 29 (20) ◽  
pp. 1450097 ◽  
Author(s):  
S. Somorendro Singh ◽  
K. K. Gupta ◽  
A. K. Jha
Keyword(s):  
Surface Tension ◽  
Critical Temperature ◽  
Droplet Size ◽  
Quark Gluon Plasma ◽  
Mean Field ◽  
Field Potential ◽  
Gluon Plasma ◽  
Loop Correction ◽  
The Mean ◽  
Mean Field Potential

Surface tension of quark–gluon plasma (QGP) evolution with one-loop correction in the mean-field potential is studied. First, with the correction, the stable QGP droplet size decreases. Then, the value of surface tension is found to be improved and it approaches to the lattice value of surface tension [Formula: see text]. Moreover, the ratio of the surface tension to the cube of the critical temperature is found to increase the value in comparison to earlier studies without correction factor [R. Ramanathan, K. K. Gupta, A. K. Jha and S. S. Singh, Pram. J. Phys. 68, 757 (2007)].

Dependence of flow behaviour of nematics in shear on the form of the mean-field potential

1993 ◽  
Vol 2 (6) ◽  
pp. 863-873
Author(s):  
Mario Minale ◽  
Giuseppe Apuzzo ◽  
Francesco Greco ◽  
Giuseppe Marrucci
Keyword(s):  
Mean Field ◽  
Field Potential ◽  
Flow Behaviour ◽  
The Mean ◽  
Mean Field Potential

SEARCH FOR THE TRI-AXIAL HEXADECAPOLE-DEFORMATION EFFECTS IN TRANS-ACTINIDAE NUCLEI

2005 ◽  
Vol 14 (03) ◽  
pp. 383-388 ◽  
Author(s):  
J. DUDEK ◽  
K. MAZUREK ◽  
B. NERLO-POMORSKA
Keyword(s):  
Dimensional Space ◽  
Mean Field ◽  
Field Potential ◽  
Nuclear Potential ◽  
Hartree Fock ◽  
Deformation Parameters ◽  
In Trans ◽  
The Mean ◽  
Mean Field Potential ◽  
Shell Energy

We have performed calculations of the nuclear potential energies in a 5-dimensional space of deformation parameters including α20, α22, α40, α42 and α44 multipole deformations by using the macroscopic-microscopic method. The energy expression contains the macroscopic term (in our case in the form of the Lublin Strasbourg Drop – LSD) and the microscopic terms of the Strutinsky shell energy and projected BCS pairing energy. The single-particle energies are obtained from the classical mean-field potential as well as from the correspondig Dirac relativistic realisation of the mean-field, both parametrised with the help of the deformed Woods-Saxon forms. Our resuls are compared to the selfconsistent Hartree Fock Bogolubov method with the D1S Gogny force.

Role of dispersion potential anisotropy in the theory of nematic liquid crystals. I. The mean‐field potential

1990 ◽  
Vol 92 (10) ◽  
pp. 6225-6234 ◽  
Author(s):  
Clark P. Eldredge ◽  
Holly T. Heath ◽  
Bruno Linder ◽  
Robert A. Kromhout
Keyword(s):  
Liquid Crystals ◽  
Nematic Liquid Crystals ◽  
Mean Field ◽  
Field Potential ◽  
The Mean ◽  
Mean Field Potential

ON THE AVERAGE PAIRING ENERGY IN NUCLEI

2007 ◽  
Vol 16 (02) ◽  
pp. 328-336 ◽  
Author(s):  
BOŻENA NERLO-POMORSKA ◽  
KRZYSZTOF POMORSKI
Keyword(s):  
Energy Dependence ◽  
Single Particle ◽  
Mean Field ◽  
Field Potential ◽  
Pairing Energy ◽  
Microscopic Method ◽  
Nucleon Number ◽  
Mean Field Potential

The macroscopic-microscopic method is applied to calculate the nuclear energies, especially the microscopic shell and pairing corrections. The single-particle levels are obtained with the Yukawa folded mean-field potential. The macroscopic energy is evaluated using the Lublin-Strasbourg Drop model. The shell corrections are obtained using the Strutinsky method with smoothing in nucleon number space. The average nuclear pairing energy is also determined by folding the BCS sums in nucleon number space. The average pairing energy dependence on the nuclear elongation is investigated.

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