| 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. c3$h-M(jVJ 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. 251^>x.R [attachment=24292] $Q cr \E3evU
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io{uN/!X_J b;XUv4~V Preface LCMCpEtY*K 1 Elements of probability theory qvH7 otA 1.1 Definitions g-Y2U}& 1.2 Properties of probabilities Ow\dk^\-G8 1.2.1 Joint probabilities #}Qzu~ 1.2.2 Conditional probabilities "Wz#<! .r 1.2.3 Bayes'theorem on inverse probabilities /X_g[*]? 1.3 Random variables and probability distributions lSzLR~=Au 1.3.1 Transformations ofvariates }t^N|I 1.3.2 Expectations and moments M{ mdh\ 1.3.3 Chebyshev inequality =6sL}$ 1.4 Generating functions ,>rr|O 1.4.1 Moment generating function wtY*{m2 1.4.2 Characteristic function cnR.J
1.4.3 Cumulants <-1(G1v 1.5 Some examples of probability distributions "V;5Lp b 1.5.1 Bernoulli or binomial distributiou mu?6Phj 1.5.2 Poisson distribution "
tUS>c/ 1.5.3 Bose-Einstein distribution Uz`K#Bz
1.5.4 The weak law of large numbers [?vn>
…… ?!:$Z4G 2 Random processes @1w9!\7Vt 3 Some useful mathematical techniques UtebSQ+h\ 4 Second-order Coherence theory of scalar wavefields Q8kdX6NMd& 5 Radiation form sources of any state of coherence m6
)s X& 7 Some applications of second-order coherence theory IP 9{vk 8 Higher-order correlations in optical fields dDAIfe2y 9 Semiclassical theory of photoelectric detection of light :q
xd])- 10 Quantization of the free electromagnetic field 61W
ms@D% 11 Coherent states of the electromagnetic field X(Wd 12 Quantum correlations and photon statistics !e}LB%zf 13 Radiation from thermal equilibrium sources ;%_fQNFb 14 Quantum theory of photoelectric detection of light \[Dxg`;4
15 Interaction between light and a two-level atom 2$g3ABfV 16 Collective atomic interactions LXIQpD,M 17 Some general techniques for treating interacting systems Uo!#p'<w)p 18 The single-mode laser &{Zt(%\ ' 19 The two-mode ring laser
YtzB/q8I 20 Squeezed states of light fJb<<6C 22 Some quantum effects in nonlinear optics B|~tW21 References B4yC"55 Author index }CiB+ Subject index >0W:snNK 0
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