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2
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0004165302
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Springer-Verlag, Berlin
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G. S. Agarwal, Quantum Optics (Springer-Verlag, Berlin, 1974), pp. 93–97.
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(1974)
Quantum Optics
, pp. 93-97
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Agarwal, G.S.1
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3
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0002890374
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JPAMA4
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D. A. Cardimona, M. G. Raymer, and C. R. Stroud, Jr., J. Phys. B 15, 55 (1982).JPAMA4
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(1982)
J. Phys. B
, vol.15
, pp. 55
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Cardimona, D.A.1
Raymer, M.G.2
Stroud, C.R.3
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5
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84926869575
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EULEEJ
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G. Grynberg and M. Pinard, Europhys. Lett. 1, 129 (1986). The authors use a similar decay scheme to investigate the influence of such a decay scheme on four-wave-mixing line shapes.EULEEJ
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(1986)
Europhys. Lett.
, vol.1
, pp. 129
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Grynberg, G.1
Pinard, M.2
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13
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0000997003
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PLRAAN
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H. Lee, P. Polynkin, M. O. Scully, and S.-Y. Zhu, Phys. Rev. A 55, 4454 (1997).PLRAAN
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(1997)
Phys. Rev. A
, vol.55
, pp. 4454
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Lee, H.1
Polynkin, P.2
Scully, M.O.3
Zhu, S.-Y.4
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14
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85037202804
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APCPCS
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V. I. Savchenko, A. A. Pantaleev, and A. N. Sarostin, in Proceedings of the 13th International Conference on Laser Interactions and Related Plasma Phenomena, edited by George Miley and E. Michael Campbell, AIP Conf. Proc. No. 406 (AIP, Woodbury, NY, 1997), p. 431.APCPCS
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(1997)
Proceedings of the 13th International Conference on Laser Interactions and Related Plasma Phenomena AIP Conf. Proc.
, pp. 431
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Savchenko, V.I.1
Pantaleev, A.A.2
Sarostin, A.N.3
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15
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6144271117
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PRLTAO
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H.-R. Xia, C.-Y. Ye, and S.-Y. Zhu, Phys. Rev. Lett. 77, 1032 (1996).PRLTAO
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(1996)
Phys. Rev. Lett.
, vol.77
, pp. 1032
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16
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21344449359
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POPTAN
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For a review of coherent population trapping see E. Arimondo, Prog. Opt. 35, 257 (1996).POPTAN
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(1996)
Prog. Opt.
, vol.35
, pp. 257
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Arimondo, E.1
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17
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4243302739
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PLRAAN
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For a discussion of this topic see D. A. Cardimona and C. R. Stroud, Jr., Phys. Rev. A 27, 2456 (1983). Cardimona and Stroud suggest that appropriate level schemes may also be found in excited states of high-Z hydrogenic ions and in multielectron atoms, but give no specific examples.PLRAAN
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(1983)
Phys. Rev. A
, vol.27
, pp. 2456
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Cardimona, D.A.1
Stroud, C.R.2
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18
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85037186488
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If the levels b and d are separated by a radio frequency, one can replace the static field by a radio-frequency field. In that case one sets (Formula presented) and replaces V by the Rabi frequency of the rf field (assuming the Rabi frequency is much less than (Formula presented)
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If the levels b and d are separated by a radio frequency, one can replace the static field by a radio-frequency field. In that case one sets (Formula presented) and replaces V by the Rabi frequency of the rf field (assuming the Rabi frequency is much less than (Formula presented).
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19
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85037240364
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Suppression of spontaneous emission still occurs if states (Formula presented) and (Formula presented) correspond to the same physical state (see Sec. III)
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Suppression of spontaneous emission still occurs if states (Formula presented) and (Formula presented) correspond to the same physical state (see Sec. III).
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22
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0031188367
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PHTOAD
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For a review see S. E. Harris, Phys. Today 50(7), 36 (1997).PHTOAD
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Phys. Today
, vol.50
, pp. 36
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Harris, S.E.1
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23
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85037178226
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Normally, the reduction of scattering in a single direction does not constitute evidence for the vacuum coupling of the excited states. The scattering must vanish in all directions. For example, if an incident field is tuned between the (Formula presented) and (Formula presented) states of Na, there can be a total suppression of scattering for specific directions and polarizations of the scattered field, even though there is no vacuum coupling of these states. The decrease in scattering in some directions is compensated for by an increase in other directions. In the experiment of Xia et al., however, the existence of scattering in the triplet channel offers proof that states (Formula presented) and (Formula presented) each contain an admixture of singlet and triplet states; as such, each can be coupled to states (Formula presented) (or (Formula presented), leading to a vacuum coupling of states (Formula presented) and (Formula presented)
-
Normally, the reduction of scattering in a single direction does not constitute evidence for the vacuum coupling of the excited states. The scattering must vanish in all directions. For example, if an incident field is tuned between the (Formula presented) and (Formula presented) states of Na, there can be a total suppression of scattering for specific directions and polarizations of the scattered field, even though there is no vacuum coupling of these states. The decrease in scattering in some directions is compensated for by an increase in other directions. In the experiment of Xia et al., however, the existence of scattering in the triplet channel offers proof that states (Formula presented) and (Formula presented) each contain an admixture of singlet and triplet states; as such, each can be coupled to states (Formula presented) (or (Formula presented), leading to a vacuum coupling of states (Formula presented) and (Formula presented)
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