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Volumn 16, Issue 7-8, 2007, Pages 439-528

A new look at the quantum mechanics of the harmonic oscillator

(1)  Kastrup, H A a  

a DESY   (Germany)

Author keywords

Angle and action variables; Harmonic oscillator; Quantum mechanics; Quantum optics

Indexed keywords

ALGEBRA; ELECTRIC FIELDS; OSCILLATORS (ELECTRONIC); QUANTUM OPTICS;

EID: 34547673150     PISSN: 00033804     EISSN: 15213889     Source Type: Journal    
DOI: 10.1002/andp.200610245     Document Type: Article
Times cited : (19)

References (323)
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    • G. Herzberg, Molecular Spectra and Molecular Structure, I. Spectra of Diatomic Molecules, 2nd edition (Litton Educational Publ., Inc., New York, 1950; afterwards publ. by Van Nostrand Reinhold Co., New York; republished by Krieger Publ. Co., Malabar, Fl., USA, 1989), Chaps.111,2, IV,2 and IV,3. I owe the reference to these discussions by Herzberg on the experimental verifications of the HO ground state energy to one of my teachers, the late Fritz Bopp, who drew our attention to that book during my time as a PhD student at the University of Munich around 1960.
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    • P. Jordan, Z. Phys. 44, 1 (1927); Jordan here quotes Dirac as telling him that he (Dirac) actually needed only the operator relation exp iφÎ- Îexp iφ = -ℏ exp iφ instead of the contradictory φ Î -Î φ = iℏ! Jordan does not mention the additional important condition Î > 0.
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    • in the present context the second paper is the most essential one. N.B. It appears to me that F. London's important contributions to the early development of quantum mechanics have been underrated and still are. He was also the first to formulate the gauge principle in quantum mechanics (Z. Phys. 42,375 (1927)),
    • in the present context the second paper is the most essential one. N.B. It appears to me that F. London's important contributions to the early development of quantum mechanics have been underrated and still are. He was also the first to formulate the gauge principle in quantum mechanics (Z. Phys. 42,375 (1927)),
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    • long before Weyl sanctioned London's quantum mechanical reinterpretation of Weyl's unsuccesful gauge theoretical extension of Einstein's General Relativity (H. Weyl, Naturwissenschaften 19, 49 (1931)).
    • long before Weyl sanctioned London's quantum mechanical reinterpretation of Weyl's unsuccesful gauge theoretical extension of Einstein's General Relativity (H. Weyl, Naturwissenschaften 19, 49 (1931)).
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    • As to the life and scientific work of F. London see K. Gavroglu, Fritz London, a scientific biography (Cambridge Univ. Press, Cambridge etc., 1995).
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    • for the radial (s-wave) case q = r ≥ 0 one has to choose appropriate boundary conditions at r = 0 (D. ter Haar, Phys. Rev. 70, 222 (1946)).
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    • For more details see [13], Appendix B.
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    • As to orbifolds see Sects. 1.4 and A.3 of [13] and the references quoted there.
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    • 1/p = exp[n In ζ- (1/p) In ζ(n + 1)], takes for In ζ(x + 1) the usual asymptotic expansion (see, e.g. [46], Sect. 8.34) and then determines the saddle point.
    • 1/p = exp[n In ζ- (1/p) In ζ(n + 1)], takes for In ζ(x + 1) the usual asymptotic expansion (see, e.g. [46], Sect. 8.34) and then determines the saddle point.
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    • The 3rd enlarged and improved Russian edition (Asimptotičeskie ocenki i celye funkcii, Moskva, 1979) contains also the estimate (512), with the factor √p missing (Chap. IV, pp. 289-294).
    • The 3rd enlarged and improved Russian edition (Asimptotičeskie ocenki i celye funkcii, Moskva, 1979) contains also the estimate (512), with the factor √p missing (Chap. IV, pp. 289-294).
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    • [104], p. 79, formula (1).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.