arXiv · 2504.09806
Quantum theory from classical mechanics near equilibrium
Abstract
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.
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Albert Schwarz. 2025-04-14. Quantum theory from classical mechanics near equilibrium. https://arxiv.org/abs/2504.09806
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