Coherence and Quantum Optics VII: Proceedings of the Seventh by Claude Cohen-Tannoudji (auth.), Joseph H. Eberly, Leonard

Optics

By Claude Cohen-Tannoudji (auth.), Joseph H. Eberly, Leonard Mandel, Emil Wolf (eds.)

The 7th Rochester convention on Coherence and Quantum Optics used to be hung on the campus of the collage of Rochester in the course of the four-day interval June 7 - 10, 1996. greater than 280 scientists from 33 international locations participated. This e-book comprises the complaints of the assembly. This convention differed from the former six within the sequence in having just a restricted variety of oral shows, in an effort to steer clear of too many parallel classes. one other new characteristic was once the creation of educational lectures. so much contributed papers have been offered in poster periods. The convention was once backed by way of the yank actual Society, via the Optical Society of the USA, by way of the foreign Union of natural and utilized Physics and via the collage of Rochester. we want to show our appreciation to those firms for his or her aid and we in particular expand our due to the foreign Union of natural and utilized Physics for offering monetary suggestions to a couple of audio system from 3rd global nations, to allow them to participate within the meeting.

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Additional resources for Coherence and Quantum Optics VII: Proceedings of the Seventh Rochester Conference on Coherence and Quantum Optics, held at the University of Rochester, June 7–10, 1995

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At this point, four remarks are in order. 1 v V V 50 r 100 Fig. 99, b) Ap = 1. 10 1) It is wpll known that there is a class of nonlinear opti('al systems, the behavior of which presents an analogy with spcond order phase tramitions in equilibriuJ1l systems. 21 for the casp of the laser; also the oro bplongs to this class. We observe that our results, especially the divergence of tl1f' correlation length as threshold is approached, represent a necessary completion to this analogy, because they add the spatial elements which were absent in the previous discussion of the problem.

A . (submitted). [12] A. G. Kofman and G. Kurizki. (preprint). [13] S. 1. McCall and E. L. Hahn. Rev 183, 457 (1969). [14] A. Maimistov, A. Basharov, and S. Rep. 191,2 (1990). [15] B. I. Mantsyzov and R. N. Kuz'min. SOY. Phys. JETP 64,37 (1986). [16] T. I. Lakoba, Phys. Lett. 'i5 (1994). ~171 R. Inguva and C. M. A 41 . 1670 (1990). r1i1] M. r. Shaw and B. W. JOSA B 8. 1127 (1991). [19J A. Kozhekin and G. Kurizki. ers 74, 5020 (1995). [20] Z. Cheng and G. hese proceedings. 34 SYNTHESIS OF ENTANGLED ATOMIC STATES AND QUANTUM COMPUTATION T.

Ed resonance interaction. III. e "engineering"). For a given photon number n in the mode, and a very slow atom, the system is described by two adiabatic field-dressed states. , ~. :3). ==> /\ ' k:> Y. /\ ,1g> A V V Y. ··· A /\ Y. V / Ejl) A "- EJI) FIG. 3. Interfering periodic non adiabatic transitions at the field nodes. , It has made a transition from the lower to the upper adiabatic state, then we find that the initial Fock-state amplitudes en are now multiplied by the amplitude An of the nonadiabatic transition at a single node.

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