Quantum charges of harmonic oscillators
- URL: http://arxiv.org/abs/2404.01756v2
- Date: Wed, 10 Apr 2024 12:45:29 GMT
- Title: Quantum charges of harmonic oscillators
- Authors: Alexander D. Popov,
- Abstract summary: We show that the energy eigenfunctions $psi_n$ with $nge 1$ are complex coordinates on orbifolds $mathbbR2/mathbbZ_n$.
We also discuss "antioscillators" with opposite quantum charges and the same positive energy.
- Score: 55.2480439325792
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: We discuss Riemannian geometry of one-dimensional quantum harmonic oscillator. Its wavefunction is a holomorphic section of the complex line bundle $L_{\sf{v}}$ over the phase space $\mathbb{R}^2$. We show that the energy eigenfunctions $\psi_n$ with $n\ge 1$, corresponding to the energy levels $E_n$, are complex coordinates on orbifolds $\mathbb{R}^2/\mathbb{Z}_n$ embedded into $L_{\sf{v}}$, where $\mathbb{Z}_n$ is the cyclic group of order $n$. In fact, $\psi_n (t,z)$ is a standing wave on $\mathbb{R}^2/\mathbb{Z}_n$, where $z$ is a complex coordinate on the phase space $\mathbb{R}^2\cong\mathbb{C}$. Oscillators are characterized by two quantum charges $(q_l^{}, q_{\sf{v}})=(n,1)$, where $q_l^{}=n$ is the winding number for the group U(1) acting on $\mathbb{R}^2/\mathbb{Z}_n$ and $q_{\sf{v}}^{}=1$ is the winding number for the U(1)-rotations on fibres of the bundle $L_{\sf{v}}\to\mathbb{R}^2$, and $E_n=\hbar\omega(q_l^{}+\frac{1}{2} q_{\sf{v}}).$ We also discuss "antioscillators" with opposite quantum charges and the same positive energy.
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