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click here Revised and up-to-date, this moment variation first explains heuristically the physics of acousto-optics prior to proposing the maths of the formal conception. the fabric is built-in to demonstrate and advertise the advance of recent principles, ideas, theories, innovations and units. The textual content additionally bargains sections at the Near-Bragg regime and curved sound wave fronts, assurance of the numerical technique, chosen purposes, assurance of anisotropic Bragg diffraction, and fabric on spectral formalisms.

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60. Lean, E. G. , Quate, C. , and Shaw, H. , Appl. Phys. , IO, 48 (1967). 61. Collins, J. , Lean, E. G. J. Appl. Phys. , 11, 240 (1967). 62. , Ireland, C, L. , and Ley, J. M. Electro-Optic and AcoustoOptic Scanning and Deflection,Marcel Dekker, New York (1983). 63. , Appl. , 3, 1577 (1969). 6 4 . , Lotsoff, S. , Proc ZEEE, 57, 160 (1969). 65. , Appl. , 21. 3624 (1 982). 66. Kroll, N. , Phys. , 127, 1207 (1962). 67. Cohen, M. , Bell System Tech. l, 44, 693 (1965). 68. , App. Phys. , 9, 425 (1966).

In their first experiment, they still useda conventional schlieren stop; later, Hiedemann [73] made use of the fact that ray bending already created an amplitude image, as predicted by Bachem and co-workers [74]. But even without ray bending, a diffraction image (Fresnel image) exists in front the of sound cell, as was first demonstratedby Nomoto [75]. The latter’s technique has been used in a modern setting by Maloney [76]and by Korpel, Laub, and Sievering [77l. Returning now to Bragg diffraction imaging, in order to explain the method more satisfactorily, it was necessary to develop a plane-wave weak interaction theory for arbitrary sound and light fields.

A particularly ingenious and beautiful method of displayingtwodimensional lociof sound velocities in any direction and for any of the three modes of sound propagation inarbitrary crystals was developed by Schaefer and Bergmann in 1934 [40]. It was based on exciting sound waves in as many modes and asmany directions as possible by the useof a crystal of somewhat irregular shape. The resulting diffracted beams (one for each mode and direction) were focused in the back focal plane of a lens. In this plane then, each pointof light correspondsto a particular mode ina specific direction.

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