Titlebook: Elements of Quantum Optics; Pierre Meystre,Murray Sargent Textbook 19901st edition Springer-Verlag Berlin Heidelberg 1990 Laser Physics.La

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Classical Nonlinear Optics,tion becomes too large for the medium to continue to respond linearly. We have already seen how a nonlinearity plays an essential role in the free electron laser pendulum equation (1.131). In another example that we discuss in detail in Chap. 6, the output intensity of a laser oscillator builds up u

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Quantum Mechanical Background,when this approach is justified and what to do when it isn’t. Unexcited systems interacting with radiation far from the system resonances can often be treated purely classically. The response of systems near and at resonance often deviates substantially from the classical descriptions. Since the las

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Mixtures and the Density Operator,the equations of motion for the probability amplitudes. However two important kinds cannot: upper to lower level decay, and more rapid decay of the electric dipole than the average level decay rate. For these two damping mechanisms, we need a more general description than can be provided by the stat

bifurcate

CW Field Interactions,atrix is extended in a form known as the ., which treats collections of atomic responses simply. Section 5-1 deals with homogeneously-broadened media, while Sec. 5-2 includes inhomogeneous broadening. The induced polarization is used as a source in the slowly-varying Maxwell equations to yield a non

易发怒

Introduction to Laser Theory,interaction of radiation with two-level atoms. We consider arrangements of two or three highly reflecting mirrors that form cavities as shown in Fig. 6-1. Light in these cavities leaks out (decays to its 1/. value) in a time . where . is the frequency of the light and . is the cavity quality factor

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Optical Bistability,output frequencies, imposed by the self-consistent laser equations, are compromises between the atomic and cavity natural frequencies. In this chapter, we discuss another situation involving a nonlinear medium in Fabry-Perot and ring cavities, but with two major changes: 1) the cavity output depends

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Saturation Spectroscopy,ility, etc. Alternatively one can use them to study the properties of the medium that generates them. The various kinds of nonlinear spectroscopy fall into the second category. Saturation spectroscopy deals typically with the . absorption of waves passing through a medium to be studied. In the simpl

Longitude

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