Abstract
For the linear effect in classes 4, ¯4, 4∶2, 4 · m, 6, 6∶2, and 6 m, one of the optic axes always coincides with the high-order symmetry axis c when the electric field e lies in a plane perpendicular to that axis, while the other describes a circular cone around c as e rotates in that plane. The same rotation in classes 3, 3∶2, 3 · m, 3 ∶ m, and m · 3 ∶ m causes both optic axes to deviate from c to opposite sides by equal angles, both describing circular cones. One of the optic axes always coincides with c for any direction of e in classes 4∶2 and 6∶2, while the other axis describes an elliptic cone around c as e rotates in a plane inclined to c. Both optic axes describe an elliptic cone in classes 3 ∶ m, 3∶2, and m · 3 ∶ m.
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References
L. M. Barkovskii and F. I. Fedorov, Kristallografiya,10, 74, 1965.
F. I. Fedorov and L. M. Barkovskii, ZhPS [Journal of Applied Spectroscopy],3, 83, 1965.
F. I. Fedorov, Optics of Anisotropic Media [in Russian], Izd. AN BSSR, Minsk, 1958.
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Barkovskii, L.M. Electrooptical parameters of uniaxial crystals. J Appl Spectrosc 6, 222–226 (1967). https://doi.org/10.1007/BF00606341
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DOI: https://doi.org/10.1007/BF00606341