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Volumn 54, Issue 6, 1996, Pages 5299-5312

Multilevel quantum beats: An analytical approach

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000281183     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.54.5299     Document Type: Article
Times cited : (101)

References (76)
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    • For a review of vibrational wave packets in molecular physics see, e.g., M. Gruebele and A. Zewail, Phys. Today 43, 24 (1990);
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    • General aspects of the dynamics of wave packets in atomic, molecular, and quantum optical systems are discussed in a review article by I. Sh. Averbukh and N. F. Perel'man, Usp. Fiz. Nauk 161, 41 (1991) [Sov. Phys. Usp. 34, 572 (1991)].
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    • For the use of fractional revivals to demonstrate the self-interference of an electron, see M. Noel, Jr. and C. R. Stroud, Phys. Rev. Lett. 75, 1252 (1995).
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    • For the phenomenon of Jaynes-Cummings revivals in the quantum motion of ions in a Paul trap, see C. A. Blockley, D. F. Walls and H. Risken, Europhys. Lett. 17, 509 (1992);
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    • In the context of classical optics, a similar phenomenon is known as the Talbot effect: Here, it represents the self-imaging of a grating, which is illuminated by plane waves, in the near field. This effect was first observed by H. F. Talbot, Philos. Mag. 9, 401 (1836).
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    • Just recently, this effect was also demonstrated for atomic waves;
    • and explained much later by L. Rayleigh, Philos. Mag. 11, 196 (1881). Just recently, this effect was also demonstrated for atomic waves;
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    • Omitted end note
    • Omitted end note.
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    • Omitted end note
    • Omitted end note.
  • 69
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    • This method was already employed successfully by different authors; see, e.g., 6,7,30
    • This method was already employed successfully by different authors; see, e.g., 6,7,30.
  • 71
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    • For a similar technique to treat the integral, fractional, and fractal Talbot effect, see M. V. Berry (unpublished) and M. V. Berry and S. Klein (unpublished)
    • For a similar technique to treat the integral, fractional, and fractal Talbot effect, see M. V. Berry (unpublished) and M. V. Berry and S. Klein (unpublished).
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    • Here we follow the definition of M. V. Berry and K. E. Mount, Rep. Prog. Phys. 35, 315 (1972) or J. Heading, An Introduction to Phase Integral Methods (Methuen, London, 1962). In contrast, C. M. Bender and S. A. Orszag, Advanced Mathematical Methods for Scientists and Engineers (McGraw-Hill, Singapore, 1984), p. 116 refer to the anti-Stokes lines defined by arg(z)=±π/3 and arg(z)=π as Stokes lines.
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    • Berry, M.V.1    Mount, K.E.2
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    • Omitted end note
    • Omitted end note.
  • 74
    • 85037245170 scopus 로고    scopus 로고
    • In the case of Rydberg atoms with eigenfrequencies ω(n)∝-1/(Formula presented) as well as in the Jaynes-Cummings model with Rabi frequencies ω(n)∝(Formula presented) we have (Formula presented)=+1
    • In the case of Rydberg atoms with eigenfrequencies ω(n)∝-1/(Formula presented) as well as in the Jaynes-Cummings model with Rabi frequencies ω(n)∝(Formula presented) we have (Formula presented)=+1.
  • 75
    • 85037205948 scopus 로고    scopus 로고
    • Omitted end note
    • Omitted end note.
  • 76
    • 0001270422 scopus 로고    scopus 로고
    • For the prediction of higher-order (fractional) revivals beyond the time scale (Formula presented), see O. Knospe and R. Schmidt, Phys. Rev. A 54, 1154 (1996).
    • (1996) Phys. Rev. A , vol.54 , pp. 1154
    • Knospe, O.1    Schmidt, R.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.