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Volumn 60, Issue 1, 1999, Pages 582-592

Numerical simulations of atomic decay in cavities and material media

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EID: 0038174994     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.60.582     Document Type: Article
Times cited : (61)

References (54)
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    • For the state of the art of the cavity QED and for references, see papers in Advances in Atomic, Molecular and Optical Physics, edited by P. R. Berman (Academic Press, New York, 1994), Suppl. 2
    • For the state of the art of the cavity QED and for references, see papers in Advances in Atomic, Molecular and Optical Physics, edited by P. R. Berman (Academic Press, New York, 1994), Suppl. 2.
  • 11
    • 85037253223 scopus 로고    scopus 로고
    • We note here that the electromagnetic mode itself is specified by the “global” structure of the cavity. This means that even though the energy from the atom (the local particle) to the field is transferred locally, the particular field mode becomes “instantly” excited in the whole cavity
    • We note here that the electromagnetic mode itself is specified by the “global” structure of the cavity. This means that even though the energy from the atom (the local particle) to the field is transferred locally, the particular field mode becomes “instantly” excited in the whole cavity.
  • 13
    • 85037182434 scopus 로고
    • Z. Phys.see also earlier work by L. Landau, 45, 340 (1927) in which the exponential decay of an atomic state due to the spontaneous emission was described for the first time.
    • (1927) , vol.45 , pp. 340
    • Landau, L.1
  • 14
    • 5844357275 scopus 로고
    • For a more detailed account of this approach, see also the monograph by C. Cohen-Tannoudji, J. Dupont-Roc, and G. Grynberg, Atom-Photon Interactions: Basic Processes and Applications (Wiley, New York, 1992)
    • J. Hamilton, Proc. Phys. Soc. London 59, 917 (1947).For a more detailed account of this approach, see also the monograph by C. Cohen-Tannoudji, J. Dupont-Roc, and G. Grynberg, Atom-Photon Interactions: Basic Processes and Applications (Wiley, New York, 1992).
    • (1947) Proc. Phys. Soc. London , vol.59 , pp. 917
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    • Proc. R. Soc. London, Ser. AG. Barton410, 141 (1987)
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    • Proc. R. Soc. London, Ser. AG. Barton410, 175 (1987).
    • (1987) , vol.410 , pp. 175
    • Barton, G.1
  • 28
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    • It is well known (see, for instance, Ref. 28) that a necessary condition for a pure exponential decay is that the energy spectrum of the electromagnetic field has no lower bound. Obviously, this is not the case of electromagnetic field neither in the free space nor in a cavity. Consequently, exponential decay is an approximation (but a very useful approximation). Deviations from exponential decay have been extensively discussed by many authors; see Refs. 1314 and P. L. Knight and P. W. Milonni, Phys. Lett. 56A, 275 (1976).
    • (1976) Phys. Lett. , vol.56A , pp. 275
    • Knight, P.L.1    Milonni, P.W.2
  • 31
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    • Phys. Rev. Lett.S. John, 58, 2486 (1987).
    • (1987) , vol.58 , pp. 2486
    • John, S.1
  • 32
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    • J. Opt. Soc. Am. B 10 (2) (1993), special issue on photonic band structures; J. Mod. Opt. 41, 171 (1994), special issue on photonic band structures
    • J. Opt. Soc. Am. B 10 (2) (1993), special issue on photonic band structures;J. Mod. Opt. 41, 171 (1994), special issue on photonic band structures.


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