cyqdesign |
2010-01-29 23:42 |
光学相干性和量子光学,作者:(L.Mandel) E.Wolf
Prior to the development of the first lasers in the 1960s, optical coherence was not a subject with which many scientists had much acquaintance, even though early contributions to the field were made by several distinguished physicists, including Max you Lane, Erwin Schrodinger and Frits Zernike. However, the situation changed once it was realized that the remarkable properties of laser light depended on its coherence. An earlier development that also triggered interest in optical coherence was a series of important experiments by Hanbury Brown and Twiss in teh 1950s,showing that, correlations between the fluctuations of mutually coherent beams of thermal light could be measured by photoelectric correlation and two-photon coincidence counting experiments. The interpretation of these experiments was, however, surrounded by controversy, which emphasized the need for understanding the coherence properties of light and their effect on the interaction between light and matter. =h0vdi%{ Prior to the development of the first lasers in the 1960s, optical coherence was not a subject with which many scientists had much acquaintance, even though early contributions to the field were made by several distinguished physicists, including Max you Lane, Erwin Schrodinger and Frits Zernike. However, the situation changed once it was realized that the remarkable properties of laser light depended on its coherence. An earlier development that also triggered interest in optical coherence was a series of important experiments by Hanbury Brown and Twiss in teh 1950s,showing that, correlations between the fluctuations of mutually coherent beams of thermal light could be measured by photoelectric correlation and two-photon coincidence counting experiments. The interpretation of these experiments was, however, surrounded by controversy, which emphasized the need for understanding the coherence properties of light and their effect on the interaction between light and matter. 4P jC[A* [attachment=24292] ,4:=n$e 0 UE8j8U'L 市场价:¥190.00 ;`Nh@*_ 优惠价:¥152.00 为您节省:38.00元 (80折) 6S`0<Z;;/ MH=7(15R P9`R~HO'` Preface I+=+ ,iXhB 1 Elements of probability theory NNt
n 1.1 Definitions wXjidOd$ 1.2 Properties of probabilities Lq|>n[KY 1.2.1 Joint probabilities /sfJ:KP0 1.2.2 Conditional probabilities &AN1xcx\ 1.2.3 Bayes'theorem on inverse probabilities X NgcBSD 1.3 Random variables and probability distributions $=iw<B r 1.3.1 Transformations ofvariates F+"_] 1.3.2 Expectations and moments 84vd~Cf9 1.3.3 Chebyshev inequality 8N%nG(
0 1.4 Generating functions yQuL[#p 1.4.1 Moment generating function nl
qn:[BU 1.4.2 Characteristic function f(Y_<% 1.4.3 Cumulants jUE gu 1.5 Some examples of probability distributions #l ZK_N|1x 1.5.1 Bernoulli or binomial distributiou LRVcf 1.5.2 Poisson distribution p}^5ru 1.5.3 Bose-Einstein distribution +? h}e 1.5.4 The weak law of large numbers d{"-iw)t …… Y8zTw`:V 2 Random processes 6|zhqb|s 3 Some useful mathematical techniques .^?zdW 4 Second-order Coherence theory of scalar wavefields Pg%9hejf3 5 Radiation form sources of any state of coherence =j62tDS 7 Some applications of second-order coherence theory L-T,[;bl 8 Higher-order correlations in optical fields P.}d@qD{) 9 Semiclassical theory of photoelectric detection of light LWyr 10 Quantization of the free electromagnetic field _dJ(h6%3 11 Coherent states of the electromagnetic field JVYH b 60Z 12 Quantum correlations and photon statistics L5-|-PP|; 13 Radiation from thermal equilibrium sources HeOdCr-PN 14 Quantum theory of photoelectric detection of light yO q@w!xz 15 Interaction between light and a two-level atom bC/":+s& p 16 Collective atomic interactions U[@y8yN6M 17 Some general techniques for treating interacting systems 1u
9hA~rj 18 The single-mode laser xG9Sk 19 The two-mode ring laser *'?7OL 20 Squeezed states of light rO'DT{Yt 22 Some quantum effects in nonlinear optics u^1#9bAW8 References >]\I:T Author index o4);5~1l Subject index Bq q=2lj :?>7Z6 市场价:¥190.00 j/FLEsU!R 优惠价:¥152.00 为您节省:38.00元 (80折) c0qp-=^&.
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