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in the limit of high detuning
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The experimental situation which most closely resembles the system we analyze here is described in T. Sleator, T. Pfau, V. Balykin, O. Carnal and J. Mlynek, Phys. Rev. Lett. 68, 1996 (1992), in the limit of high detuning.
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25
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See, for example, D. S. Saxon, Elementary Quantum Mechanics (Holden-Day, San Francisco, 1968), pp. 144–147. The algebra becomes especially simple if Eq. (3.7) is interpreted as a squeezed state
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See, for example, D. S. Saxon, Elementary Quantum Mechanics (Holden-Day, San Francisco, 1968), pp. 144–147. The algebra becomes especially simple if Eq. (3.7) is interpreted as a squeezed state.
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26
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85037201004
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For a thorough discussion see, for instance, R. Rubenstein, Term Paper (for a class in Atomic Physics), Massachusetts Institute of Technology, 1995 (unpublished)
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For a thorough discussion see, for instance, R. Rubenstein, Term Paper (for a class in Atomic Physics), Massachusetts Institute of Technology, 1995 (unpublished).
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27
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See, for instance, P. E. Moskowitz, P. L. Gould and D. Pritchard, J. Opt. Soc. Am. B 2, 1784 (1985);
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31
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85037184000
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Increasing the interaction time may help as well, but the growing influence of diffusive processes on the deterioration of fringe visibility is not easy to foresee. The best compromise between large T and a small spontaneous aberration may be found empirically by gradually slowing down the atomic beam
-
Increasing the interaction time may help as well, but the growing influence of diffusive processes on the deterioration of fringe visibility is not easy to foresee. The best compromise between large T and a small spontaneous aberration may be found empirically by gradually slowing down the atomic beam.
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32
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3843146888
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33
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2242491318
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We do not claim here that the particular setup described in 25 can be used for this purpose. In particular, a significant birefringence of the cavity prevents the realization of two-state atomic dynamics, as mentioned, in H. Mabuchi, Q. A. Turchette, M. S. Chapman and H. J. Kimble, Opt. Lett. 21, 1393 (1995).
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85037184256
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Cooling of Cs atoms below the one-photon recoil limit has been demonstrated in traps. See, for instance, C. Salomon, J. Dalibard, W. D. Philips, A. Clairon, and S. Guellati, Europhys. Lett. 12(8), 638 (1990);
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Cooling of Cs atoms below the one-photon recoil limit has been demonstrated in traps. See, for instance, C. Salomon, J. Dalibard, W. D. Philips, A. Clairon, and S. Guellati, Europhys. Lett. 12(8), 638 (1990);
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