Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 263
... optic axis , because in these cases one can study optical activity free from the effects of ordinary birefringence . We must now ask : if this effect can occur when light is transmitted along an optic axis in bire- fringent crystals ...
... optic axis , because in these cases one can study optical activity free from the effects of ordinary birefringence . We must now ask : if this effect can occur when light is transmitted along an optic axis in bire- fringent crystals ...
Page 273
Their Representation by Tensors and Matrices John Frederick Nye. along the optic axes , and so manifestations of optical activity must be sought in other directions ; in case ( 2 ) the symmetry allows rotation along the optic axes but it ...
Their Representation by Tensors and Matrices John Frederick Nye. along the optic axes , and so manifestations of optical activity must be sought in other directions ; in case ( 2 ) the symmetry allows rotation along the optic axes but it ...
Page 274
... Optical activity in uniaxial and biaxial crystals in directions inclined to the optic axes . In a crystal that is both optically active and ordinarily birefringent there are , for any wave normal , two waves that are transmitted ...
... Optical activity in uniaxial and biaxial crystals in directions inclined to the optic axes . In a crystal that is both optically active and ordinarily birefringent there are , for any wave normal , two waves that are transmitted ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
EQUILIBRIUM PROPERTIES | 51 |
ELECTRIC POLARIZATION | 68 |
18 other sections not shown
Common terms and phrases
angle anisotropic applied axial vector centre of symmetry Chapter coefficients conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dielectric dijk direction cosines dummy suffix elastic electric field ellipsoid equation example force given grad H₁ H₂ heat flow Hence hexagonal homogeneous indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization principal axes produced pyroelectric pyroelectric effect quantities radius vector referred refractive index relation representation quadric represented right-handed rotation S₁ scalar second-rank tensor set of axes shear strain stress suffix notation surface susceptibility symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values x₁ Young's Modulus zero