Analysis of the single-particle energies of 1f and 2p proton states in 64,66,68Zn nuclei by the mean field model with dispersive optical potential

2011 ◽  
Vol 75 (7) ◽  
pp. 883-884 ◽  
Author(s):  
O. V. Bespalova ◽  
T. A. Ermakova ◽  
A. A. Klimochkina ◽  
E. A. Romanovsky ◽  
T. I. Spasskaya
Keyword(s):  
Single Particle ◽  
Optical Potential ◽  
Field Model ◽  
Mean Field ◽  
Mean Field Model ◽  
Dispersive Optical Potential ◽  
The Mean

Calculation of single-particle energies in the 38 96 Sr nucleus within the mean field model with the dispersive optical potential

2009 ◽  
Vol 73 (11) ◽  
pp. 1442-1445 ◽  
Author(s):  
O. V. Bespalova ◽  
I. N. Boboshin ◽  
V. V. Varlamov ◽  
B. S. Ishkhanov ◽  
E. A. Romanovskii ◽  
...  
Keyword(s):  
Single Particle ◽  
Optical Potential ◽  
Field Model ◽  
Mean Field ◽  
Mean Field Model ◽  
Dispersive Optical Potential ◽  
The Mean

Investigation of the shell structure of 40 ⩽ A ⩽ 132 magic and near-magic nuclei within the mean-field model involving a dispersive optical potential

2009 ◽  
Vol 72 (10) ◽  
pp. 1629-1638 ◽  
Author(s):  
O. V. Bespalova ◽  
I. N. Boboshin ◽  
V. V. Varlamov ◽  
T. A. Ermakova ◽  
B. S. Ishkhanov ◽  
...  
Keyword(s):  
Shell Structure ◽  
Optical Potential ◽  
Field Model ◽  
Mean Field ◽  
Mean Field Model ◽  
Dispersive Optical Potential ◽  
The Mean

Single-Crystal Magnetic Properties of [Co(NH3)5(OH2)] [Cr(CN)6] Between 2 and 300 K

1992 ◽  
Vol 45 (11) ◽  
pp. 1899 ◽  
Author(s):  
PA Reynolds ◽  
CD Delfs ◽  
BN Figgis ◽  
B Moubaraki ◽  
KS Murray
Keyword(s):  
Ising Model ◽  
Field Model ◽  
Mean Field ◽  
Zero Field ◽  
Spin Orbit Coupling ◽  
Zero Field Splitting ◽  
Magnetic Exchange Interaction ◽  
Mean Field Model ◽  
Magnetic Exchange ◽  
The Mean

The magnetic susceptibilities along and perpendicular to the c axis (hexagonal setting) between 2.0 and 300 K at a magnetic field of 1.00 T, and the magnetizations at field strengths up to 5.00 T, are presented for single crystals of [Co(NH3)5(OH2)] [Cr(CN)6]. The results are interpreted in terms of zero-field splitting (2D) of the ground 4A2g term by spin-orbit coupling and of magnetic exchange interaction between the chromium atoms. The magnetic exchange is modelled as one of Ising or mean-field in type. The exchange is found to be quite small: J = -0.18(6) cm-1 if the Ising model is employed, and -0.03(1) cm-1 for the mean-field model. The model adopted for the exchange has a strong influence on the value of the parameter D obtained. When the Ising model is used D is deduced to be -0.28(9) cm-l; when the mean-field model is used D is -0.14(4) cm-l. The g-values deduced are in agreement with those from e.s.r. measurements at higher temperatures and do not depend on the exchange model. In any case, D is found to be sufficiently large that it must be considered in a polarized neutron diffraction experiment on the compound.

scholarly journals Phase diagram of the mean field model of simplicial gravity

1999 ◽  
Vol 542 (1-2) ◽  
pp. 413-424 ◽  
Author(s):  
P. Bialas ◽  
Z. Burda ◽  
D. Johnston
Keyword(s):  
Phase Diagram ◽  
Field Model ◽  
Mean Field ◽  
Mean Field Model ◽  
The Mean
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