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Brillouin scattering
Vacher, R. and Courtens, E.  International Tables for Crystallography (2013). Vol. D, ch. 2.4, pp. 349-355 [ doi:10.1107/97809553602060000914 ]
... stress component is also produced by the internal electric field E, so that the constitutive equation (2.4.2.2) has an additional term (see Section 1.1.5.2 ), where e is the piezoelectric tensor at constant strain. The electrical displacement vector D, related to E by the dielectric tensor , also contains a contribution from ...

Use of the tables
Vacher, R. and Courtens, E.  International Tables for Crystallography (2013). Vol. D, Section 2.4.5, p. 351 [ doi:10.1107/97809553602060000914 ]
Use of the tables 2.4.5. Use of the tables The tables in this chapter give information on modes and scattering geometries that are in most common use in the study of hypersound in single crystals. Just as in the case of X-rays, Brillouin scattering is not sensitive to the presence ...

Scattering cross section
Vacher, R. and Courtens, E.  International Tables for Crystallography (2013). Vol. D, Section 2.4.4.2, pp. 350-351 [ doi:10.1107/97809553602060000914 ]
Scattering cross section 2.4.4.2. Scattering cross section The power , scattered from the illuminated volume V in a solid angle , where and are measured inside the sample, is given by where is the incident light intensity inside the material, is the appropriate elastic constant for the observed phonon, and the factor results ...
     [more results from section 2.4.4 in volume D]

Coupling via the electro-optic effect
Vacher, R. and Courtens, E.  International Tables for Crystallography (2013). Vol. D, Section 2.4.3.2, p. 350 [ doi:10.1107/97809553602060000914 ]
Coupling via the electro-optic effect 2.4.3.2. Coupling via the electro-optic effect Piezoelectric media also exhibit an electro-optic effect linear in the applied electric field or in the field-induced crystal polarization. This effect is described in terms of the third-rank electro-optic tensor r defined by Using ...
     [more results from section 2.4.3 in volume D]

Piezoelectric media
Vacher, R. and Courtens, E.  International Tables for Crystallography (2013). Vol. D, Section 2.4.2.2, pp. 349-350 [ doi:10.1107/97809553602060000914 ]
... stress component is also produced by the internal electric field E, so that the constitutive equation (2.4.2.2) has an additional term (see Section 1.1.5.2 ), where e is the piezoelectric tensor at constant strain. The electrical displacement vector D, related to E by the dielectric tensor , also contains a contribution from ...
     [more results from section 2.4.2 in volume D]

Introduction
Vacher, R. and Courtens, E.  International Tables for Crystallography (2013). Vol. D, Section 2.4.1, p. 349 [ doi:10.1107/97809553602060000914 ]
... Doctoral Thesis, University of Montpellier. Cummins, H. Z. & Schoen, P. E. (1972). Linear scattering from thermal fluctuations. In Laser handbook, Vol. 2, edited by F. T. Arecchi & E. O. Schulz-Dubois, pp. 1029-1075. Amsterdam: North-Holland. Egelstaff ... xenon single crystals. Solid State Commun. 8, 1529-1533. Gross, E. (1930a). Change of wave-length of light due ...

Techniques of Brillouin spectroscopy
Vacher, R. and Courtens, E.  International Tables for Crystallography (2013). Vol. D, Section 2.4.6, pp. 351-355 [ doi:10.1107/97809553602060000914 ]
... is unequalled in its frequency range. References Born, M. & Wolf, E. (1993). Principles of optics. Sixth corrected edition. Oxford: Pergamon ... Fabry-Perot interferometer. Appl. Opt. 7, 951-966. Mach, J. E., McNutt, D. P., Roessler, F. L. & Chabbal, R. (1963). ...

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