The anisotropic harmonic oscillator in a magnetic field

1972 ◽  
Vol 5 (1) ◽  
pp. 1-4 ◽  
Author(s):  
T. K. Rebane
2008 ◽  
Vol 77 (5) ◽  
Author(s):  
J. I. Jiménez-Aquino ◽  
R. M. Velasco ◽  
F. J. Uribe

1992 ◽  
Vol 07 (38) ◽  
pp. 3593-3600
Author(s):  
R. CHITRA

The properties of the ground state of N anyons in an external magnetic field and a harmonic oscillator potential are computed in the large-N limit using the Thomas-Fermi approximation. The number of level crossings in the ground state as a function of the harmonic frequency, the strength and the direction of the magnetic field and N are also studied.


1971 ◽  
Vol 14 (4) ◽  
pp. 492-495 ◽  
Author(s):  
I. M. Ternov ◽  
V. G. Bagrov ◽  
V. N. Zadorozhnyi

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.


2019 ◽  
Vol 54 (2) ◽  
pp. 023002
Author(s):  
K H Raveesha ◽  
S Suma ◽  
R Ranjitha ◽  
R Rakshitha

Author(s):  
Gleb L. Kotkin ◽  
Valeriy G. Serbo

This chapter addresses the adiabatic invariant for a mathematical pendulum, a model of a “gas” consisting of a single molecule in a piston, adiabatic approximation, and a simplified model of an ion H2+. The chapter also discusses the connection between the volume and the pressure of a gas consisting of particles inside an elastic cube, the adiabatic invariants for a charged anisotropic harmonic oscillator in a uniform magnetic field, a magnetic trap, and the action and angle variables for the simple systems.


Author(s):  
Gleb L. Kotkin ◽  
Valeriy G. Serbo

This chapter addresses the canonical transformation defined by the given generating function, the rotation in the phase space as a canonical transformation, and themovement of the system as a canonical transformation. The chapter also discusses using the canonical transformations for solving the problems of the anharmonic oscillations and using the canonical transformation to diagonalize the Hamiltonian function of an anisotropic charged harmonic oscillator in a magnetic field. Finally, the chapter addresses the canonical variables which reduce the Hamiltonian function of the harmonic oscillator to zero and using them for consideration of the system of the harmonic oscillators with the weak nonlinear coupling.


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