Titlebook: Nonlinear Optics; Basic Concepts D. L. Mills Textbook 19911st edition Springer-Verlag Berlin Heidelberg 1991 Laser.Nichtlineare Optik.chemi

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书目名称Nonlinear Optics影响因子(影响力)




书目名称Nonlinear Optics影响因子(影响力)学科排名




书目名称Nonlinear Optics网络公开度




书目名称Nonlinear Optics网络公开度学科排名




书目名称Nonlinear Optics被引频次




书目名称Nonlinear Optics被引频次学科排名




书目名称Nonlinear Optics年度引用




书目名称Nonlinear Optics年度引用学科排名




书目名称Nonlinear Optics读者反馈




书目名称Nonlinear Optics读者反馈学科排名

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, and the condensed phases of matter. A parallel development, readily detectable in the recent literature of theoretical physics, has been the substantial advance in OUf understand­ ing of highly nonlinear phenomena. Numerous texts are devoted to exposition of the theoretical methods which may be used to extr978-3-662-00213-1

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Introductory Remarks,ll always be concerned with electric fields whose spatial variation involves length scales very large compared to the size of the atoms and molecules that are the basic constituents of the material of interest. In this regard, we note that in the visible portion of the spectrum, the wavelength of li

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Linear Dielectric Response of Matter,moment per unit volume displayed in (1.7 b). For much of what follows here, the tensor nature of the dielectric response is of little explicit interest, so we assume for the moment the dielectric susceptibility tensor .. introduced in Chap. 1 is diagonal, .. = ....

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Interaction of Atoms with Nearly Resonant Fields: Self-Induced Transparency,an be expanded in powers of the electric field .. The justification for this procedure is the notion that the largest applied fields encountered in practice are very small compared to those encountered by an electron within an atom or a molecule. It follows that the electronic arrangement in the ato

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Self-Interaction Effects in One-Dimensional Wave Propagation: Solitons in Optical Fibers and in Pernic structure of the physical system exposed to the electromagnetic field is perturbed far from equilibrium in the course of its evolution. In the soliton pulses encountered in the theory of self-induced transparency, for example, the resonant atoms are moved from their ground state, to the first ex

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Chaos,ies. Our first example was the response of the anharmonic oscillator described by (3.15). This led us to understand, on the basis of this simple model, the qualitative aspects of the frequency variation of the nonlinear susceptibilities, and also the influence of the anharmonic terms on the frequenc

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