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Pauli's theorem and quantum canonical pairs: the consistency of a bounded, self-adjoint time operator canonically conjugate to a Hamiltonian with non-empty point spectrum

机译:保利定理和量子正则对:有界,自伴时间算子对非空点谱哈密顿量的典型共轭一致性

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In single Hilbert space, Pauli's well-known theorem implies that the existence of a self-adjoint time operator canonically conjugate to a given Hamiltonian requires the Hamiltonian to possess completely continuous spectra spanning the entire real line. Thus the conclusion that there exists no self-adjoint time operator conjugate to a semibounded or discrete Hamiltonian despite some well-known illustrative, implicit counterexamples. In this paper we evaluate Pauli's theorem against the single Hilbert space formulation of quantum mechanics, and consequently show the consistency of assuming a bounded, self-adjoint time operator canonically conjugate to a Hamiltonian with an unbounded, or semibounded, or finite point spectrum. We point out Pauli's implicit assumptions and show that they are not consistent. We demonstrate our analysis by giving two explicit examples. Moreover, we clarify issues surrounding the different solutions to the canonical commutation relations, and, consequently, expand the class of acceptable canonical pairs beyond the solutions required by Pauli's theorem. [References: 49]
机译:在单个希尔伯特空间中,保利的著名定理意味着,一个自伴时间算子的存在与给定的哈密顿量典范共轭,要求哈密顿量具有完全连续的,跨越整个实线的光谱。因此,尽管存在一些众所周知的说明性隐式反例,但结论是不存在与半界或离散哈密顿量共轭的自伴时间算子。在本文中,我们针对量子力学的单个希尔伯特空间公式对保利定理进行了评估,因此证明了假设有界,自伴时间算符正则共轭到具有无界,半界或有限点谱的哈密顿量的一致性。我们指出了Pauli的隐含假设,并表明它们不一致。我们通过给出两个明确的例子来证明我们的分析。此外,我们阐明了围绕典型换向关系的不同解决方案的问题,因此,扩展了可接受的经典对的类别,使其超出了Pauli定理所要求的解决方案。 [参考:49]

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