scholarly journals Atomic hydrogen in a uniform magnetic field: Low-lying energy levels for fields above109G

1987 ◽  
Vol 35 (2) ◽  
pp. 647-656 ◽  
Author(s):  
Chih-Ray Liu ◽  
Anthony F. Starace
Universe ◽  
2021 ◽  
Vol 7 (12) ◽  
pp. 467
Author(s):  
Fayçal Hammad ◽  
Alexandre Landry ◽  
Parvaneh Sadeghi

The relativistic wave equation for spin-1/2 particles in the interior Schwarzschild solution in the presence of a uniform magnetic field is obtained. The fully relativistic regime is considered, and the energy levels occupied by the particles are derived as functions of the magnetic field, the radius of the massive sphere and the total mass of the latter. As no assumption is made on the relative strengths of the particles’ interaction with the gravitational and magnetic fields, the relevance of our results to the physics of the interior of neutron stars, where both the gravitational and the magnetic fields are very intense, is discussed.


2006 ◽  
Vol 20 (32) ◽  
pp. 5417-5425
Author(s):  
HONG-YI FAN ◽  
TONG-TONG WANG ◽  
YAN-LI YANG

We show that the recently proposed invariant eigenoperator method can be successfully applied to solving energy levels of electron in an anisotropic quantum dot in the presence of a uniform magnetic field (UMF). The result reduces to the energy level of electron in isotropic harmonic oscillator potential and in UMF naturally. The Landau diamagnetism decreases due to the existence of the anisotropic harmonic potential.


2011 ◽  
Vol 25 (03) ◽  
pp. 365-370 ◽  
Author(s):  
M. R. SETARE ◽  
D. JAHANI

We examine the effect of a magnetic field that varies inversely as the square of distance on the Dirac fermion spectrum of graphene, a single layer of graphite. We find that unlike the case of the uniform magnetic field for which zero-energy modes exhibit half the degeneracy of the other levels in the energy spectrum, the ground state in this case, as well as the other energy levels, is doubly degenerate. We also get zero-energy solutions for the special case of ky = 0.


2006 ◽  
Vol 84 (9) ◽  
pp. 801-811
Author(s):  
Savely G Karshenboim

The sum rules for the energy levels of a hyperfine multiplet in a constant uniform magnetic field are presented. It is found that for any value of the electron angular moment and the nuclear spin there are certain linear combinations of energy levels that do not depend on the magnetic field and can be used to determine the unperturbed hyperfine-structure separation in the presence of a perturbing magnetic field. It is also demonstrated that there are other linear combinations that are linear with the external magnetic field and hence can be used to determine bound values of the electron and nuclear magnetic moments. The accuracy of the approximation within which the result is valid is also discussed.PACS Nos.: 32.10.Fn, 32.60.+i1


1982 ◽  
Vol 26 (3-4) ◽  
pp. 415-417 ◽  
Author(s):  
C.W. Clark ◽  
K.T. Taylor

2006 ◽  
Vol 21 (15) ◽  
pp. 3171-3179 ◽  
Author(s):  
V. R. KHALILOV ◽  
F. KH. CHIBIROVA

The behavior of an electrically charged massive particle (an electron) is studied in a constant uniform magnetic field and a single attractive λδ(r) potential. A simple transcendental equation that determines the electron energy spectrum is derived. The approximate wave function of a loosely bound state is constructed in a very simple form. The model under consideration makes it possible to study the effect of magnetic fields on a loosely bound electron. It is shown that the sizes of the electron localization region change and the probability current density arises when the electron is in the loosely bound state in the presence of a constant uniform magnetic field. The above current must involve (and exercise influence on) the electron scattering. The probability current resembles a stack of "pancake vortices" whose circulating (around the z-axes) "currents" are mostly confined within the plane z = 0 in the weak magnetic field. The equation for determining the energy levels of the electron states is obtained for the model under study in two spatial dimensions and the energy of the loosely bound state is found for the two-dimensional model.


1953 ◽  
Vol 31 (6) ◽  
pp. 1010-1014 ◽  
Author(s):  
G. Lamarche ◽  
G. M. Volkoff

A theoretical investigation is presented of the energy levels of a nucleus of spin I = 5/2, a given magnetic moment μ, and electric quadruple moment eQ, placed in a uniform magnetic field H0, and a crystalline electrostatic potential [Formula: see text] without axial symmetry. The dependence of the energy levels, line frequencies, and transition matrix elements on the dimensionless parameter [Formula: see text] is calculated for Al27 for one orientation of a spodumene crystal in the magnetic field H0 over the interesting range of the parameter R linking up the pure quadrupole with the Zeeman spectrum. Other orientations of the crystal are discussed briefly.


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