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Bibliographic Details
Main Author: Kokoulin, Radmir
Format: Preprint
Published: 2025
Subjects:
Online Access:https://arxiv.org/abs/2504.17830
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author Kokoulin, Radmir
author_facet Kokoulin, Radmir
contents We introduce a self-adjoint time operator $T_w = i\hbar\bigl(\partial_E + \tfrac12\,\partial_E\ln w(E)\bigr)$ on the weighted energy space $L^2(\mathbb R,\,w(E)\,dE)$. Under mild conditions on the weight $w$ (positivity, local absolute continuity, and uniform bounds at large $\lvert E\rvert$), we prove that $T_w$ is essentially self-adjoint. A simple unitary conjugation carries $T_w$ back to $i\hbar\,\mathrm{d}/\mathrm{d}E$, which in turn leaves the Hamiltonian spectrum unbounded.
format Preprint
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institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Self-Adjoint Time Operator in a Weighted Energy Space
Kokoulin, Radmir
Quantum Physics
We introduce a self-adjoint time operator $T_w = i\hbar\bigl(\partial_E + \tfrac12\,\partial_E\ln w(E)\bigr)$ on the weighted energy space $L^2(\mathbb R,\,w(E)\,dE)$. Under mild conditions on the weight $w$ (positivity, local absolute continuity, and uniform bounds at large $\lvert E\rvert$), we prove that $T_w$ is essentially self-adjoint. A simple unitary conjugation carries $T_w$ back to $i\hbar\,\mathrm{d}/\mathrm{d}E$, which in turn leaves the Hamiltonian spectrum unbounded.
title Self-Adjoint Time Operator in a Weighted Energy Space
topic Quantum Physics
url https://arxiv.org/abs/2504.17830