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1
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84926536978
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J. Opt. Soc. Am. B 4 (10) (1987) special issue on squeezed states of the electromagnetic field, edited by H.J. Kimble and D.F. Walls.
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2
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84926555188
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J. Mod. Opt. 34 (617) (1987) special issue on squeezed light, edited by P.L. Knight and R. Loudon.
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3
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84926547227
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Appl. Phys. B 55 (3) (1992) special issue on quantum noise reduction in optical systems, edited by C. Fabre and E. Giacobino.
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5
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84926552837
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For example, see the review by P. Meystre, in Progress in Optics, Vol. XXX, edited by E. Wolf (North Holland, Amsterdam, 1992), Chap. V.
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14
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0001444905
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The emphasis in this work is in fact on the preparation of motional Fock states of a trapped ion, but the same scheme can in principle be applied to a cavity QED configuration and to the generation of photon Fock states. More recently
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(1994)
Phys. Rev. A
, vol.49
, pp. R3174
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Cirac, J.I.1
Blatt, R.2
Zoller, P.3
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15
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84926585615
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have also proposed a scheme for the preparation of ``motional'' Fock states in an ion trap using the same adiabatic passage principle employed in the present paper.
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22
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84926535305
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See, for example, A. Messiah, Quantum Mechanics (North Holland, Amsterdam, 1962), Vol. II.
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31
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0001305144
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and by
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(1994)
Phys. Rev. Lett.
, vol.72
, pp. 997
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Goldner, L.S.1
Gerz, C.2
Spreeuw, R.J.C.3
Rolston, S.L.4
Westbrook, C.I.5
Phillips, W.D.6
Marte, P.7
Zoller, P.8
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32
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84926587325
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If we take the specific example of cesium, then frequencies are scaled in units of 2π×106 s-1, so that Γ =5 corresponds to an atomic spontaneous emission rate of 3.1×107 s-1. Suitable units of time would be (2π×106)-1 s, so that T=1 corresponds to an interaction time of 159 ns.
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33
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84926597086
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R.J. Thompson, O. Carnal, and H.J. Kimble (unpublished); H.J. Kimble, in Cavity Quantum Electrodynamics, Advances in Atomic, Molecular, and Optical Physics, Supplement 2, edited by P.R. Berman (Academic, San Diego, 1994).
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44
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84926560312
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H.J. Carmichael, L. Tian, W. Ren, and P. Alsing, in Cavity Quantum Electrodynamics, Advances in Atomic, Molecular, and Optical Physics, Supplement 2 (Ref. [27]); H.J. Carmichael, P. Kochan, and L. Tian, in Proceedings of the International Symposium on Coherent States: Past, Present, and Future (World Scientific, Singapore, in press). In these works, optimal results are obtained when the local oscillator photon flux is chosen to decay at the same rate as the signal photon flux, i.e., at the cavity mode energy loss rate; such a choice should also be desirable in any practical homodyne experiment testing the present scheme.
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46
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84926573704
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The discussion presented in this section is based upon research carried out in collaboration with H. Mabuchi.
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47
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84926563102
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For recent reviews of the status of BAE measurement, see, Ap, pl. Phys, B 55, 291 (1992) and, G. Taubes
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(1994)
Science
, vol.263
, pp. 1376
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Roch, J.F.1
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48
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84926548962
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and references therein.
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50
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0028335038
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For a recent review of ``quantum repeaters,'' see
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(1994)
Science
, vol.263
, pp. 1394
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Yamamoto, Y.1
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51
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84926549721
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and references therein.
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55
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84926566618
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have independently put forth an idea similar to the one described above but based upon a coherent Rabi oscillation at frequency g for a two level atom which transits two separated ``lobes'' of a microwave resonator.
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57
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84926591462
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in Laser Optics '93 (SPIE, Bellingham, WA, in press).
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