Rotational Symmetry and Gauge Invariant Degeneracies on 2D Noncommutative Plane
We obtain the gauge invariant energy eigenvalues and degeneracies together with rotationally symmetric wavefunctions of a particle moving on 2D noncommutative plane subjected to homogeneous magnetic field $B$ and harmonic potential. This has been done by using the phase space coordinates transformat...
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Main Authors: | , , , , |
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Format: | Journal Article |
Language: | English |
Published: |
16-12-2021
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Subjects: | |
Online Access: | Get full text |
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Summary: | We obtain the gauge invariant energy eigenvalues and degeneracies together
with rotationally symmetric wavefunctions of a particle moving on 2D
noncommutative plane subjected to homogeneous magnetic field $B$ and harmonic
potential. This has been done by using the phase space coordinates
transformation based on 2-parameter family of unitarily equivalent irreducible
representations of the nilpotent Lie group $G_{NC}$. We find that the energy
levels and states of the system are unique and hence, same goes to the
degeneracies as well since they are heavily reliant on the applied $B$ and the
noncommutativity $\theta $ of coordinates. Without $B$, we essentially have a
noncommutative planar harmonic oscillator under generalized Bopp shift or
Seiberg-Witten map. The degenerate energy levels can always be found if
$\theta$ is proportional to the ratio between $\hbar$ and $m\omega$. For the
scale $B\theta = \hbar$, the spectrum of energy is isomorphic to Landau problem
in symmetric gauge and hence, each energy level is infinitely degenerate
regardless of any values of $\theta$. Finally, if $0 < B\theta < \hbar$,
$\theta$ has to also be proportional to the ratio between $\hbar$ and $m\omega$
for the degeneracy to occur. These proportionality parameters are evaluated and
if they are not satisfied then we will have non-degenerate energy levels.
Finally, the probability densities and effects of $B$ and $\theta$ on the
system are properly shown for all cases. |
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DOI: | 10.48550/arxiv.2112.08666 |