Optics

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

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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 throughout the four-day interval June 7 - 10, 1996. greater than 280 scientists from 33 nations participated. This ebook comprises the complaints of the assembly. This convention differed from the former six within the sequence in having just a restricted variety of oral displays, so one can steer clear of too many parallel periods. one other new function used to be the advent of educational lectures. such a lot contributed papers have been offered in poster classes. The convention was once backed through the yankee actual Society, via the Optical Society of the US, through the foreign Union of natural and utilized Physics and by way of the college of Rochester. we want to convey our appreciation to those companies for his or her aid and we in particular expand our because of the foreign Union of natural and utilized Physics for supplying monetary tips to a couple of audio system from 3rd global international locations, to let them to participate within the meeting.

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Extra 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

Example text

1 umts of CIl, 2 Figure 1. Injection versus detuning plane from linear stability analysis. , N = N. l. Here the injection versus detuning plane is divided into two broad regions. The region above the lines given asymptotically by is the phase locked region denoted by (LS) and (LV), for which steady state solutions with constant phase can in principle exit. The region below these lines (FWM) is the four wave mixing region in which the solutions are periodic[5]. This designation is taken only for convenience since as we will see later in these region there exist subregions in which the solutions show very complicated behavior[5].

H and C is the cavity roundtrip length. For Wo < w" ¢L = 0 or 7r /2, usi ng the model dcscri bed in Sec. 2 one obtai ns th' following expression for the equal-time (t = t') correlation function Cdl·)6: Cdr) _ ~ . ( . [2'0)1/2 'J Cdr = 0) - 7r 1I1lho 1 kc d + lc 1, (24) where kc is the critical wave vector defined by Eq. e. 0= (1 - A;)1/2. (25) The long distance behavior of the function CL is given by r -> 00 (26) where the correlation length (27) diverges when threshold is approached (0 -> 0). Fig.

We therefore set out to complement these past measurements and theoretical calculations by examining as much as possible the injection versus detuning regime and paying particular attention to the strong injection versus large detuning region. In addition this effort will allow us to develop not only experimental methods but also numerical and analytical tools that will make it possible to attack much more complicated problems in coupled lasers and also in semiconductor lasers that show instabilities under weak feedback.

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