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Volumn 64, Issue 12, 1996, Pages 1451-1456

The uncertainty principle for energy and time

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EID: 0030523945     PISSN: 00029505     EISSN: None     Source Type: Journal    
DOI: 10.1119/1.18410     Document Type: Article
Times cited : (100)

References (22)
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    • Springer-Verlag, Berlin, These two pages provide an easy reference for the views we want to criticize in this article, but similar views are widespread in the literature
    • John von Neumann, Mathematical Foundations of Quantum Mechanics (Princeton University, Princeton, 1955), pp. 353, 354. Translated from the original German edition: Johann von Neumann, Mathematische Grundlagen der Quantenmechanik (Springer-Verlag, Berlin, 1932), pp. 187 and 188. These two pages provide an easy reference for the views we want to criticize in this article, but similar views are widespread in the literature.
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    • Von Neumann, J.1
  • 5
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    • In view of the difficulties that beset the definition of action and angle variables as self-adjoint operators in quantum mechanics we prefer the more general term "observable" to distinguish them from c numbers
    • In view of the difficulties that beset the definition of action and angle variables as self-adjoint operators in quantum mechanics we prefer the more general term "observable" to distinguish them from c numbers.
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    • i and t are functions. It is then possible to find an appropriate Lagrangian for the system. From this Lagrangian the momentum conjugate to t may be calculated and it turns out to be - H. This would then be a ground for considering t and -H as forming a fourth canonical pair. However, the next step, the inversion of the Lagrangian to obtain the generalized velocities as functions of the generalized coordinates and momenta, turns out to be impossible, that is, the equations of motion cannot be written in the usual Hamiltonian form
    • i and t are functions. It is then possible to find an appropriate Lagrangian for the system. From this Lagrangian the momentum conjugate to t may be calculated and it turns out to be - H. This would then be a ground for considering t and -H as forming a fourth canonical pair. However, the next step, the inversion of the Lagrangian to obtain the generalized velocities as functions of the generalized coordinates and momenta, turns out to be impossible, that is, the equations of motion cannot be written in the usual Hamiltonian form.
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    • Pauli has already remarked that if the spectrum of t is the whole real axis and t and H satisfy the commutation relation in (1), then the spectrum of H cannot contain discrete eigenvalues. In fact, the restrictions following from H≥0 are even more severe
    • Pauli has already remarked that if the spectrum of t is the whole real axis and t and H satisfy the commutation relation in (1), then the spectrum of H cannot contain discrete eigenvalues. In fact, the restrictions following from H≥0 are even more severe.
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    • The uncertainty relation between energy and time in nonrelativistic quantum mechanics
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    • On the energy-time uncertainty relation
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.