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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:泡利定理与量子规范对:一致性   有界,自伴随时间算子与哈密顿量的典型共轭   非空点谱

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摘要

In single Hilbert space, Pauli's well-known theorem implies that theexistence of a self-adjoint time operator canonically conjugate to a givenHamiltonian signifies that the time operator and the Hamiltonian possesscompletely continuous spectra spanning the entire real line. Thus theconclusion that there exists no self-adjoint time operator conjugate to asemibounded or discrete Hamiltonian despite some well-known illustrativecounterexamples. In this paper we evaluate Pauli's theorem against the singleHilbert space formulation of quantum mechanics, and consequently show theconsistency of assuming a bounded, self-adjoint time operator canonicallyconjugate to a Hamiltonian with an unbounded, or semibounded, or finite pointspectrum. We point out Pauli's implicit assumptions and show that they are notconsistent in a single Hilbert space. We demonstrate our analysis by giving twoexplicit examples. Moreover, we clarify issues sorrounding the differentsolutions to the canonical commutation relations, and, consequently, expand theclass of acceptable canonical pairs beyond the solutions required by Pauli'stheorem.
机译:在单个希尔伯特空间中,保利的著名定理表明,自伴随时间算子的存在与给定的哈密顿量典范共轭,这表明时间算子和哈密顿量具有跨越整个实线的完全连续谱。因此,尽管存在一些众所周知的说明性反例,但结论是不存在与半边界或离散哈密顿量共轭的自伴随时间算子。在本文中,我们根据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,因此证明了有界,自伴随时间算子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,并表明它们在单个希尔伯特空间中不一致。我们通过给出两个明显的例子来证明我们的分析。此外,我们澄清了围绕正则换向关系的不同解决方案的问题,因此,扩展了保理定理所要求的解决方案之外的可接受正则对的类别。

著录项

  • 作者

    Galapon, Eric A.;

  • 作者单位
  • 年度 2002
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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