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Titlebook: Wave Phenomena; Theoretical, Computa Lui Lam,Hedley C. Morris Conference proceedings 1989 Springer-Verlag New York Inc. 1989 Phase.electrom

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發(fā)表于 2025-3-28 18:09:27 | 只看該作者
Mario A. Fusco,Mary V. Smithm Swift has gotten into the optics act with incredible but eminently useful optical devices. Indeed, Mother Nature herself has had a hand in evolving image-maki978-3-662-14473-2978-3-540-38801-2Series ISSN 0342-4111 Series E-ISSN 1556-1534
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發(fā)表于 2025-3-28 22:00:51 | 只看該作者
Hiap Liew Ong on the above affine set, are called the cusps, because of the way they look in a fundamental domain in the upper half plane. They generate a subgroup of the di978-1-4419-2813-9978-1-4757-1741-9Series ISSN 0072-7830 Series E-ISSN 2196-9701
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Phase Space Factorization and Functional Integral Methods in Direct and Inverse Scattering — Symbol pseudo-differential and Fourier integral operators. In conjunction with the global functional integral techniques pioneered by Wiener (Brownian motion) and Feynman (quantum mechanics), and so successfully applied today in quantum field theory and statistical physics, the .-dimensional classical phy
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發(fā)表于 2025-3-29 23:43:40 | 只看該作者
Conference proceedings 1989n in random media. Part II consists of papers that involve significant amounts of computation. Included are papers on the Fast Hartley Transform, computational algorithms for electromagnetic scattering problems, and nonlinear wave interaction problems in fluid mechanics. vi Part III contains papers
49#
發(fā)表于 2025-3-30 02:48:01 | 只看該作者
The Woodward Bequestthat group at Ames for some years and also remembered Henry. As the faculty in our Department considered how best to use Mrs. Woodward’s generous gift as a memorial to her son and to continue the scientific research on which he worked, we consulted with all those people and they contributed many excellent ideas.
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發(fā)表于 2025-3-30 06:06:15 | 只看該作者
Paraxial Wave Equations and Absorbing Boundary Conditionscan serve in place of (1.1) if we are concerned only with waves propagating in some preferred direction. Solutions of (1.1) that correspond to wave propagating in the positive direction along the x-axis are solutions of the equation.and solutions propagating in the negative direction are solutions of
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