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3
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85037225201
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H.J. Carmichael, An Open Systems Approach to Quantum Optics (Springer-Verlag, Berlin, 1993)
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H.J. Carmichael, An Open Systems Approach to Quantum Optics (Springer-Verlag, Berlin, 1993).
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11
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85037240330
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C.W. Gardiner and P. Zoller, Quantum Noise, 2nd ed. (Springer-Verlag, Berlin, 2000)
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C.W. Gardiner and P. Zoller, Quantum Noise, 2nd ed. (Springer-Verlag, Berlin, 2000).
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15
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85037237560
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M.O. Scully and M.S. Zubairy, Quantum Optics (Cambridge University Press, Cambridge, 1997)
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M.O. Scully and M.S. Zubairy, Quantum Optics (Cambridge University Press, Cambridge, 1997).
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18
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85037215679
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J.D. Bjorken and S.D. Drell, Relativistic Quantum Fields (McGraw-Hill, New York, 1965), p. 12
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J.D. Bjorken and S.D. Drell, Relativistic Quantum Fields (McGraw-Hill, New York, 1965), p. 12.
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20
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85037202638
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general, the atom volume of interest is its “coherence volume.” For simplicty, we treat here the case of a pure atomic wave packet, with no loss of generality
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In general, the atom volume of interest is its “coherence volume.” For simplicty, we treat here the case of a pure atomic wave packet, with no loss of generality.
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23
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85037204146
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In the case at hand, W. M. Itano has emphasized the well-known result that for a coherent state driving field the problem is unitarily equivalent to a classical driving field plus vacuum fluctuations. W.M. Itano, e-print quant-ph/0211165; See also
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Itano, W.M.1
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26
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85037199443
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C. Cohen-Tannoudji, J. Dupont-Roc, and G. Grynberg, Atom-Photon Interactions (Wiley, New York, 1992)
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C. Cohen-Tannoudji, J. Dupont-Roc, and G. Grynberg, Atom-Photon Interactions (Wiley, New York, 1992).
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27
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85037181613
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J. Preskill, Quantum Computation Lecture Notes, 1998, Chap. 3 (unpublished), also see www.theory.caltech.edu/people/preskill/ph229/#lecture
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J. Preskill, Quantum Computation Lecture Notes, 1998, Chap. 3 (unpublished), also see www.theory.caltech.edu/people/preskill/ph229/#lecture
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36
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85037189006
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This result generalizes under the assumption that the probe detuning is large compared to the hyperfine splitting in the (Formula presented) manifold. We can use the Lande projection theorem to make the substitution (Formula presented) where F is the total ground-state angular momentum including nuclear spin
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This result generalizes under the assumption that the probe detuning is large compared to the hyperfine splitting in the (Formula presented) manifold. We can use the Lande projection theorem to make the substitution (Formula presented) where F is the total ground-state angular momentum including nuclear spin.
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