Energy levels and wave functions of Bloch electrons in rational and irrational magnetic fields

1976 ◽  
Vol 14 (6) ◽  
pp. 2239-2249 ◽  
Author(s):  
Douglas R. Hofstadter
2015 ◽  
Vol 70 (7) ◽  
pp. 499-505 ◽  
Author(s):  
Zahra Sharifi ◽  
Fateme Tajic ◽  
Majid Hamzavi ◽  
Sameer M. Ikhdair

AbstractThe Killingbeck potential model is used to study the influence of the external magnetic and Aharanov–Bohm (AB) flux fields on the splitting of the Dirac energy levels in a 2+1 dimensions. The ground state energy eigenvalue and its corresponding two spinor components wave functions are investigated in the presence of the spin and pseudo-spin symmetric limit as well as external fields using the wave function ansatz method.


1971 ◽  
Vol 3 (12) ◽  
pp. 4091-4099 ◽  
Author(s):  
H. H. Hosack ◽  
P. L. Taylor

1971 ◽  
Vol 4 (8) ◽  
pp. 2833-2833
Author(s):  
H. H. Hosack ◽  
P. L. Taylor

1992 ◽  
Vol 06 (18) ◽  
pp. 3057-3068 ◽  
Author(s):  
XIAN-GENG ZHAO ◽  
SHI-GANG CHEN

The energy spectrum and the wave functions for a tight-binding Bloch electron on coupled chains under the action of both uniform electric and magnetic fields are studied in detail. Exact results are obtained for the case when the coupling between chains is large by using the perturbation theory, from which it is found that the spectrum is that of two interspaced Stark ladders. The magnetic field dependence of the energy spectrum is also discussed.


Nanomaterials ◽  
2021 ◽  
Vol 11 (7) ◽  
pp. 1720
Author(s):  
Antonios Balassis ◽  
Godfrey Gumbs ◽  
Oleksiy Roslyak

We have investigated the α–T3 model in the presence of a mass term which opens a gap in the energy dispersive spectrum, as well as under a uniform perpendicular quantizing magnetic field. The gap opening mass term plays the role of Zeeman splitting at low magnetic fields for this pseudospin-1 system, and, as a consequence, we are able to compare physical properties of the the α–T3 model at low and high magnetic fields. Specifically, we explore the magnetoplasmon dispersion relation in these two extreme limits. Central to the calculation of these collective modes is the dielectric function which is determined by the polarizability of the system. This latter function is generated by transition energies between subband states, as well as the overlap of their wave functions.


1992 ◽  
Vol 45 (15) ◽  
pp. 8749-8751 ◽  
Author(s):  
C. Kutter ◽  
V. Chitta ◽  
J. C. Maan ◽  
V. I. Fal’ko ◽  
M. L. Leadbeater ◽  
...  

2000 ◽  
Vol 61 (15) ◽  
pp. 9879-9882 ◽  
Author(s):  
Alejandro Kunold ◽  
Manuel Torres

1987 ◽  
Vol 120 ◽  
pp. 103-105
Author(s):  
J. Le Bourlot ◽  
E. Roueff

We present a new calculation of intercombination transition probabilities between levels X1Σg+ and a 3Πu of the C2 molecule. Starting from experimental energy levels, we calculate RKR potential curves using Leroy's Near Dissociation Expansion (NDE) method; these curves give us wave functions for all levels of interest. We then compute the energy matrix for the four lowest states of C2, taking into account Spin-Orbit coupling between a 3Πu and A 1Πu on the one hand and X 1Σ+g and b 3Σg− on the other. First order wave functions are then derived by diagonalization. Einstein emission transition probabilities of the Intercombination lines are finally obtained.


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