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By Valentin G. Dmitriev, Gagik G. Gurzadyan, David N. Nikogosyan

Because the invention of the 1st laser 30 years in the past, the frequency conversion of laser radiation in nonlinear optical crystals has turn into a big method standard in quantum electronics and laser physics for fixing a number of clinical and engineering difficulties. the elemental physics of three-wave mild interactions in nonlinear optical crystals is now good understood. This has enabled the construction of varied harmonic turbines, sum-and distinction­ frequency turbines, and optical parametric oscillators in keeping with nonlinear optical crystals which are now commercially to be had. even as, scientists proceed an lively look for novel, hugely effective nonlinear optical fabrics. for this reason, in our opinion, there's a nice desire for a guide of nonlinear optical crystals, meant for experts and practitioners with an engineering history. This publication incorporates a whole description of the homes and purposes of all nonliner optical crystals of functional significance said within the literature as much as the start of 1990. furthermore, it comprises crucial equations for calculating the most parameters (such as phase-matching path, powerful nonlinearity, and conversion potency) of nonlinear frequency converters. Dolgoprudnyi, Yerevan, Troitzk v. G. Dmitriev USSR G. G. Gurzadyan October 1990 D. N. Nikogosyan Contents 1 advent. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2 Optics of Nonlinear Crystals. . . . . . . . . . . . . . . . . . . . . . . . three . . . . . .

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The problem (a) has no surface wave solutions. The problem (b) has no more than one surface wave solution. The problem (c) has no more than two surface wave solutions. The problem (d) has at least one surface wave solution (provided that the limiting wave is not exceptional) but not more than two solutions; if the limiting wave is exceptional then there could be two, one or none surface wave solutions. (156) In principle, varying ε and µ in (b)1 and (c)1 from 0 to ∞ we can obtain all possible physical situations including all the other problems in the presented list (a), (b), (c), (d).

8. The plane specified by the unit vectors m and n is known as a sagittal plane. In the chosen coordinate system the steady-state displacement field of the plane wave can be presented in the 31 Figure 8. Cross section of slowness surface sheets by a sagittal plane form of a superposition of partial waves, u(x − vt, y) = A(y) exp[ik(x − vt)], A(y) = bαAα exp(ikpαy), (125) α which have equal x -components of the wave vector, kx ≡ k, and a common tracing speed v = ω/k, but different y-components of the wave vector, (α) ky = pαk, and polarization vectors Aα.

A very significant step in the phonon-focusing investigations has been taken by Northrop & Wolfe [17, 18] who developed the alternative phonon imaging method. For the details of this method and for more extensive literature reflecting the further progress in this field, both in theory and in experiments, we refer readers to the review articles [21, 24] and to the book [25]. 4. (3)-(5), as λα, λβ and λγ , and suppose that along the direction m = md degeneracy of two of them occurs, say λα = λβ . Then, instead of (16), one can write Q(md) = λαI + (λγ − λα)Aγ ⊗ Aγ .

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