Introduction to Solid State PhysicsProblems after each chapter. |
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Page 4
... vector a ' must be of the form T , as in Eq . ( 1.3 ) . The vector a ' - a - a has the components - ay = a sin ; ax ' - ax = a ( cos & - 1 ) ; αν and so ( 1.4 ) la ' - 2 Now we must have a ' - a a2 ( 2 2 cos p ) . = - a2a2 , because a ...
... vector a ' must be of the form T , as in Eq . ( 1.3 ) . The vector a ' - a - a has the components - ay = a sin ; ax ' - ax = a ( cos & - 1 ) ; αν and so ( 1.4 ) la ' - 2 Now we must have a ' - a a2 ( 2 2 cos p ) . = - a2a2 , because a ...
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 545
... vector . It is clear that the Burgers vector must be one of a discrete set of lattice vectors that will allow the rewelding process to maintain the crystallinity of the material . The Burgers vector of a screw dislocation is parallel to ...
... vector . It is clear that the Burgers vector must be one of a discrete set of lattice vectors that will allow the rewelding process to maintain the crystallinity of the material . The Burgers vector of a screw dislocation is parallel to ...
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 levels 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 region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero