Harmonic oscillator states with integer and non-integer orbital angular momentum

Abstract

We study the quantum mechanical harmonic oscillator in two and three dimensions, with particular attention to the solutions as basis states for representing their respective symmetry groups -O(2), O(3), and O(2,1). Solving the Schrodinger equation by separating variables in polar coordinates, we obtain wavefunctions characterized by a principal quantum number, the group Casimir eigenvalue, and one observable component of orbital angular momentum, with eigenvalue m + s, for integer m and real constant parameter s. For each of the three symmetry groups, s splits the solutions into two inequivalent representations, one associated with s = 0, from which we recover the familiar description of the oscillator as a product of one-dimensional solutions, and the other with s > 0 (in three dimensions, solutions are found for s = 0 and s = 1/2) whose solutions are non-separable in Cartesian coodinates, and are hence overlooked by the standard Fock space approach. In two dimensions, a single set of creation and annihilation operators forms a ladder representation for the allowed oscillator states for any s, and the degeneracy of energy states is always finite. However, in three dimensions, the integer and half-integer eigenstates are qualitatively different: the former can be expressed as finite dimensional irreducible tensors under O(3) or O(2,1) while the latter exhibit infinite degeneracy. Creation operators that produce the allowed integer states by acting on the non-degenerate ground state are constructed as irreducible tensor products of the fundamental vector representation. However, since the half-integer ground state has infinite degeneracy, the vector representation of the creation operators does not take this ground state to the calcluated first excited level, and the general construction does not act as a ladder representation for the half-integer states. For all s = 0 solutions, the SU(N) symmetry of the harmonic oscillator Hamiltonian recently discussed by Bars is spontaneously broken by the ground state. The connection of this symmetry breaking to the non-separability into one-dimensional Cartesian solutions is demonstrated.

The Lagrangian of charged test particle in Horava-Lifshitz black hole and deformed phase space

“…( 18) with new variables in Eq. (24). Hence, the form of Hamiltonian in the deformed analysis is found as, Ĥ = 1 2…”

“…Moreover, the problem of quantum mechanics on NC spaces can be found in the context of deformed spacetime [21,22]. The NC space from the approach of deformation for harmonic oscillators is reported in [23,24].…”

Symmetry of the Relativistic Two-Body Bound State

“…There are no ghost states in the covariant treatment we discuss here, and no extra constraints invoked in finding the spectrum. The solutions are given in terms of Laguerre poynomials, but unlike the case of the standard treatment of the 4D oscillator, in which x µ ± ip µ are considered annihilation-creation operators, the spectrum generating algebra (for example, Dothan [36]) for the covariant SHP oscillator has been elusive [37].…”

Novel Outlook on the Eigenvalue Problem for the Orbital Angular Momentum Operator

“…Götte et al [7], exploiting the freedom in fixing the orientation of phase discontinuity, introduced states with non-integer angular momentum and applied formalism of the propagation of light modes with the fractional angular momentum in the paraxial and non-paraxial regime. Exploring polar solutions for the harmonic oscillator, Land [8] discovered that the Fock space equivalent to the Hilbert space wave functions, found by solving the Schrodinger equation in spherical coordinates is realized by acting with the creation and annihilation operators, allowing states with both integer and non-integer angular momentum.…”