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Auteur principal: Schwarz, Albert
Format: Preprint
Publié: 2025
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Accès en ligne:https://arxiv.org/abs/2504.09806
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_version_ 1866910913876983808
author Schwarz, Albert
author_facet Schwarz, Albert
contents We consider classical theories described by Hamiltonians $H(p,q)$ that have a non-degenerate minimum at the point where generalized momenta $p$ and generalized coordinates $q$ vanish. We assume that the sum of squares of generalized momenta and generalized coordinates is an integral of motion. In this situation, in the neighborhood of the point $p=0, q=0$ quadratic part of a Hamiltonian plays a dominant role. We suppose that a classical observer can observe only physical quantities corresponding to quadratic Hamiltonians and show that in this case, he should conclude that the laws of quantum theory govern his world.
format Preprint
id arxiv_https___arxiv_org_abs_2504_09806
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Quantum theory from classical mechanics near equilibrium
Schwarz, Albert
Quantum Physics
High Energy Physics - Theory
Mathematical Physics
81
We consider classical theories described by Hamiltonians $H(p,q)$ that have a non-degenerate minimum at the point where generalized momenta $p$ and generalized coordinates $q$ vanish. We assume that the sum of squares of generalized momenta and generalized coordinates is an integral of motion. In this situation, in the neighborhood of the point $p=0, q=0$ quadratic part of a Hamiltonian plays a dominant role. We suppose that a classical observer can observe only physical quantities corresponding to quadratic Hamiltonians and show that in this case, he should conclude that the laws of quantum theory govern his world.
title Quantum theory from classical mechanics near equilibrium
topic Quantum Physics
High Energy Physics - Theory
Mathematical Physics
81
url https://arxiv.org/abs/2504.09806