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Titlebook: Nonlinear Optics; Basic Concepts D. L. Mills Textbook 1998Latest edition Springer-Verlag Berlin Heidelberg 1998 Absorption.Faraday rotation

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21#
發(fā)表于 2025-3-25 03:55:50 | 只看該作者
D. L. Millsoncerning the estimation of key risk parameters like default probabilities. Further, a large v- ume of literature on the pricing and measurement of credit risk in a portfolio c- text has evolved. This development was partly reflected by supervisors when they agreed on the new revised capital adequac
22#
發(fā)表于 2025-3-25 07:53:11 | 只看該作者
23#
發(fā)表于 2025-3-25 13:24:15 | 只看該作者
D. L. Mills tests and their application for bank internal purposes, especially in the Basel II periphery. We built up a simulation based framework to take account of dependencies in defaults (asset correlation), which additionally has the potential to appraise the type II error, i.e. the non-detection of a bad
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發(fā)表于 2025-3-25 16:46:35 | 只看該作者
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發(fā)表于 2025-3-25 23:07:37 | 只看該作者
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發(fā)表于 2025-3-26 03:57:47 | 只看該作者
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發(fā)表于 2025-3-26 05:07:15 | 只看該作者
28#
發(fā)表于 2025-3-26 11:46:51 | 只看該作者
Interaction of Atoms with Nearly Resonant Fields: Self-Induced Transparency,their influence can be substantial, as illustrated by our model discussions of second harmonic generation, and the stimulated Raman effect. A bucket full of water may have only a small leak, but if one waits long enough, the bucket will be quite empty.
29#
發(fā)表于 2025-3-26 15:30:13 | 只看該作者
Introductory Remarks,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 light is roughly 5×10. cm, while a typical molecular bond length or crystal lattice constant is3×10.cm. We may then proceed by studying the solutions of Maxwell’s equations, which have the form
30#
發(fā)表于 2025-3-26 20:14:06 | 只看該作者
Self-Interaction Effects in One-Dimensional Wave Propagation: Solitons in Optical Fibers and in Periton pulses encountered in the theory of self-induced transparency, for example, the resonant atoms are moved from their ground state, to the first excited state, at the midpoint of the pulse. We now return to the regime of weak nonlinearities, where the nonlinear polarization P. may be expanded in powers of the electric field.
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