132Te and single-particle density-dependent pairing

Author(s):  
N. V. Zamfir ◽  
R. O. Hughes ◽  
R. F. Casten ◽  
D. C. Radford ◽  
C. J. Barton ◽  
...  
2005 ◽  
Vol 25 (S1) ◽  
pp. 389-390
Author(s):  
N. V. Zamfir ◽  
R. O. Hughes ◽  
R. F. Casten ◽  
D. C. Radford ◽  
C. J. Barton ◽  
...  

2004 ◽  
Vol 69 (5) ◽  
Author(s):  
R. O. Hughes ◽  
N. V. Zamfir ◽  
R. F. Casten ◽  
D. C. Radford ◽  
C. J. Barton ◽  
...  

1981 ◽  
Vol 53 (1) ◽  
pp. 95-126 ◽  
Author(s):  
Anjuli S. Bamzai ◽  
B. M. Deb

2014 ◽  
Vol 28 (03) ◽  
pp. 1450046
Author(s):  
B. H. J. McKELLAR

In a particular exactly solvable model of an interacting system, the Boltzmann equation predicts a constant single particle density operator, whereas the exact solution gives a single particle density operator with a nontrivial time dependence. All of the time dependence of the single particle density operator is generated by the correlations.


1995 ◽  
Vol 09 (22) ◽  
pp. 1407-1417 ◽  
Author(s):  
ALEXANDER MOROZ

The single-particle densitity of states (DOS) for the Pauli and the Schrödinger Hamiltonians in the presence of an Aharonov–Bohm potential is calculated for different values of the particle magnetic moment. The DOS is a symmetric and periodic function of the flux. The Krein–Friedel formula can be applied to this long-ranged potential when regularized with the zeta function. We have found that whenever a bound state is present in the spectrum it is always accompanied by a resonance. The shape of the resonance is not of the Breit-Wigner type. The differential scattering cross section is asymmetric if a bound state is present and gives rise to the Hall effect. As an application, propagation of electrons in a dilute vortex limit is considered and the Hall resistivity is calculated.


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