Time Operators of Harmonic Oscillators and Their Representations

Fuente: arXiv
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Main Authors: Hiroshima, Fumio, Teranishi, Noriaki
Format: Preprint
Published: 2022
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author Hiroshima, Fumio
Teranishi, Noriaki
author_facet Hiroshima, Fumio
Teranishi, Noriaki
contents A time operator $\hat T_\eps$ of the one-dimensional harmonic oscillator $ \hat h_\eps=\half(p^2+\eps q^2)$ is rigorously constructed. It is formally expressed as $ \hat T_\eps=\half\frac{1}{\sqrt \eps } (\arctan (\sqrt \eps \hat t_0)+\arctan (\sqrt \eps \hat t_1))$ with $\hat t_0=p^{-1}q$ and $\hat t_1=qp^{-1}$. It is shown that the canonical commutation relation $[h_\eps, \hat T_\eps ]=-i\one$ holds true on a dense domain in the sense of sesqui-linear forms, and the limit of $\hat T_\eps $ as $\eps\to 0$ is shown. Finally a matrix representation of $\hat T_\eps$ and its analytic continuation are given.
format Preprint
id arxiv_https___arxiv_org_abs_2201_06352
institution arXiv
publishDate 2022
record_format arxiv
spellingShingle Time Operators of Harmonic Oscillators and Their Representations
Hiroshima, Fumio
Teranishi, Noriaki
Mathematical Physics
A time operator $\hat T_\eps$ of the one-dimensional harmonic oscillator $ \hat h_\eps=\half(p^2+\eps q^2)$ is rigorously constructed. It is formally expressed as $ \hat T_\eps=\half\frac{1}{\sqrt \eps } (\arctan (\sqrt \eps \hat t_0)+\arctan (\sqrt \eps \hat t_1))$ with $\hat t_0=p^{-1}q$ and $\hat t_1=qp^{-1}$. It is shown that the canonical commutation relation $[h_\eps, \hat T_\eps ]=-i\one$ holds true on a dense domain in the sense of sesqui-linear forms, and the limit of $\hat T_\eps $ as $\eps\to 0$ is shown. Finally a matrix representation of $\hat T_\eps$ and its analytic continuation are given.
title Time Operators of Harmonic Oscillators and Their Representations
topic Mathematical Physics
url https://arxiv.org/abs/2201.06352