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 Results for DC.creator="A." AND DC.creator="M." AND DC.creator="Glazer" in section 1.6.7 of volume D
The acousto-optic effect
Glazer, A. M. and Cox, K. G.  International Tables for Crystallography (2013). Vol. D, Section 1.6.7.3, pp. 178-179 [ doi:10.1107/97809553602060000905 ]
... optic effect The acousto-optic effect (Sapriel, 1976) is really a variant of the elasto-optic effect, in that the strain field is created by the passage of a sound wave through the crystal. If this wave has frequency , the resulting polarization in the presence of a light wave of frequency is given by , where . ...

Spontaneous strain in BaTiO3
Glazer, A. M. and Cox, K. G.  International Tables for Crystallography (2013). Vol. D, Section 1.6.7.2, pp. 177-178 [ doi:10.1107/97809553602060000905 ]
... transition of the well known perovskite BaTiO3. This substance undergoes a transition at around 403K on cooling from its high-temperature ... both ferroelectric and ferroelastic. In this tetragonal phase, there is a small distortion of the unit cell along [001] and a contraction along compared with the unit cell of the ...

Introduction
Glazer, A. M. and Cox, K. G.  International Tables for Crystallography (2013). Vol. D, Section 1.6.7.1, pp. 176-177 [ doi:10.1107/97809553602060000905 ]
... in terms of the change in dielectric impermeability caused by a static (or low-frequency) field, in this case a stress, applied to the crystal. This can be written in the form The coefficients form a fourth-rank tensor known as the linear piezo-optic ...

The linear photoelastic effect
Glazer, A. M. and Cox, K. G.  International Tables for Crystallography (2013). Vol. D, Section 1.6.7, pp. 176-179 [ doi:10.1107/97809553602060000905 ]
... in terms of the change in dielectric impermeability caused by a static (or low-frequency) field, in this case a stress, applied to the crystal. This can be written in the form The coefficients form a fourth-rank tensor known as the linear piezo-optic ...

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