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G. S. Agarwal, Quantum Statistical Theories of Spontaneous Emission and Their Relation to Other Approaches, edited by G. Möhler et al. Springer Tracts in Modern Physics: Quantum Optics Vol. 70 (Springer-Verlag, Berlin, 1974), Sec. 15.
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For studies of such coherence effects in the context of (Formula presented) system see J. Javanainen, Europhys. Lett. 17, 407 (1992)
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H. Lee, P. Polynkin, M. O. Scully, and S. Y. Zhu, Phys. Rev. A 55, 4454 (1997).
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M. A. G. Martinez, P. R. Herczfeld, C. Samuels, L. M. Narducci, and C. H. Keitel, Phys. Rev. A 55, 4483 (1997)
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0030284210
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We also note that several other methods have been suggested in the literature to overcome the problem of orthogonal dipole matrix elements. These include the application of dc, rf, or even optical fields depending on the situationation at hand. Here the nonorthogonality is obtained from mixing of energy levels. The details can be found in H. Schmidt and A. Imamoğlu, Opt. Commun. 131, 333 (1996)
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Coherence effects in the context of the decay of nuclear levels are discussed in R. Coussement, M. V. Bergh, G. S’heeren, G. Neyens, and R. Nouwen, Phys. Rev. Lett. 71, 1824 (1993).
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For more recent reviews on this subject, see J. J. Childs, Kyungwon An, R. R. Dasari, and M. S. Feld, in Cavity Quantum Electrodynamics, edited by P. R. Berman (Academic, New York, 1993), p. 325
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For an excellent review and references on theories and experiments on cavity induced changes of spontaneous emission, see S. Haroche and D. Kleppner, Phys. Today 42 (1), 24 (1989).For more recent reviews on this subject, see J. J. Childs, Kyungwon An, R. R. Dasari, and M. S. Feld, in Cavity Quantum Electrodynamics, edited by P. R. Berman (Academic, New York, 1993), p. 325.
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B. M. Garraway and P. L. Knight, [Phys. Rev. A 54, 3592 (1996)] examined the modifications in quantum beats of a V system, where the system is placed in a cavity and is prepared in a coherent superposition of two excited states.
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