Tables for
Volume D
Physical properties of crystals
Edited by A. Authier

International Tables for Crystallography (2006). Vol. D, ch. 2.4, p. 330

Section Kinematics

R. Vachera* and E. Courtensa

aLaboratoire des Verres, Université Montpellier 2, Case 069, Place Eugène Bataillon, 34095 Montpellier CEDEX, France
Correspondence e-mail: Kinematics

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Brillouin scattering occurs when an incident photon at frequency [\nu _i] interacts with the crystal to either produce or absorb an acoustic phonon at [\delta \nu], while a scattered photon at [\nu _s] is simultaneously emitted. Conservation of energy gives [\delta \nu = \nu _s - \nu _i, \eqno (]where positive [\delta \nu] corresponds to the anti-Stokes process. Conservation of momentum can be written [{\bf Q}= {\bf k}_s - {\bf k}_i, \eqno (]where Q is the wavevector of the emitted phonon, and [{\bf k}{_s}], [{\bf k}{_i}] are those of the scattered and incident photons, respectively. One can define unit vectors q in the direction of the wavevectors k by [\eqalignno{{\bf k}_i &= 2\pi {\bf q}n/\lambda _0, & ( \cr {\bf k}_s &= 2\pi {\bf q}'n'/\lambda _0, &(}]where n and [n'] are the appropriate refractive indices, and [\lambda _0] is the vacuum wavelength of the radiation. Equation ([link] assumes that [\delta \nu \ll \nu _i] so that [\lambda _0] is not appreciably changed in the scattering. The incident and scattered waves have unit polarization vectors [{\bf e}] and [{\bf e}'], respectively, and corresponding indices n and [n']. The polarization vectors are the principal directions of vibration derived from the sections of the ellipsoid of indices by planes perpendicular to [{\bf q}] and [{\bf q}'], respectively. We assume that the electric vector of the light field Eopt is parallel to the displacement Dopt. This is exactly true for many cases listed in the tables below. In the other cases (such as skew directions in the orthorhombic group) this assumes that the birefringence is sufficiently small for the effect of the angle between [{\bf E}_{\rm opt}] and [{\bf D}_{\rm opt}] to be negligible. A full treatment, including this effect, has been given by Nelson et al. (1972[link]).

After substituting ([link] in ([link], the unit vector in the direction of the phonon wavevector is given by [\hat{\bf Q}= {{n'{\bf q}' - n{\bf q}}\over {\left| {n'{\bf q}' - n{\bf q}}\right|}}. \eqno (]The Brillouin shift [\delta \nu] is related to the phonon velocity V by [\delta \nu = VQ/2\pi. \eqno (]Since [\nu \lambda _0 = c], from ([link] and ([link], ([link] one finds [\delta \nu \cong (V/{\lambda _0 }) [{n^2 + ({n'} )^2 - 2nn'\cos \theta } ]^{1/2}, \eqno (]where [\theta ] is the angle between [{\bf q}] and [{\bf q}'].


Nelson, D. F., Lazay, P. D. & Lax, M. (1972). Brillouin scattering in anisotropic media: calcite. Phys. Rev. B, 6, 3109–3120.Google Scholar

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