Introduction to Solid State PhysicsProblems after each chapter. |
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Page 4
... vector a ' a must be of the form T , as in Eq . ( 1.3 ) . The vector a ' - a has the components ax ' - ах = a ( cos & - 1 ) ; αν ay = a sin p ; and so ( 1.4 ) a ' - a2 = a2 ( 2 - 2 cos p ) . Now we must have a ' - is the shortest vector ...
... vector a ' a must be of the form T , as in Eq . ( 1.3 ) . The vector a ' - a has the components ax ' - ах = a ( cos & - 1 ) ; αν ay = a sin p ; and so ( 1.4 ) a ' - a2 = a2 ( 2 - 2 cos p ) . Now we must have a ' - is the shortest vector ...
Page 50
... vector r * ( hkl ) in the reciprocal lattice is in the same direction but n times as long as the vector corresponding to the true crystal plane . That is , the nth point from the origin in a given row in the reciprocal lattice ...
... vector r * ( hkl ) in the reciprocal lattice is in the same direction but n times as long as the vector corresponding to the true crystal plane . That is , the nth point from the origin in a given row in the reciprocal lattice ...
Page 544
... vector distance b , which may be arbitrarily oriented relative to the surface . Forces will be required to effect the displacement . The medium is filled in or cut away so as to be continuous after the displacement . It is then joined ...
... vector distance b , which may be arbitrarily oriented relative to the surface . Forces will be required to effect the displacement . The medium is filled in or cut away so as to be continuous after the displacement . It is then joined ...
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