Introduction to Solid State PhysicsProblems after each chapter. |
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Page 102
... direction with particle motion along a [ 110 ] direction in a cubic crystal is v = [ ( c11 - C12 ) / 2pol . 4.6 . Show that in a cubic crystal the condition for a longitudinal wave in the [ 111 ] direction to have the same velocity as a ...
... direction with particle motion along a [ 110 ] direction in a cubic crystal is v = [ ( c11 - C12 ) / 2pol . 4.6 . Show that in a cubic crystal the condition for a longitudinal wave in the [ 111 ] direction to have the same velocity as a ...
Page 428
... direction , refer- red to the lower energy required to saturate along a direction of easy magnetization . The excess energy required in the hard direction is the anisotropy energy . As an example of anisotropy energy we may consider ...
... direction , refer- red to the lower energy required to saturate along a direction of easy magnetization . The excess energy required in the hard direction is the anisotropy energy . As an example of anisotropy energy we may consider ...
Page 431
... direction cosines of the magnetization direction referred to the cubic axes , and B1 , B2 , B3 are the direction cosines of the direction in which ôl is measured ; A100 and A111 are the saturation values of the longitudinal ...
... direction cosines of the magnetization direction referred to the cubic axes , and B1 , B2 , B3 are the direction cosines of the direction in which ôl is measured ; A100 and A111 are the saturation values of the longitudinal ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero