Introduction to Solid State PhysicsProblems after each chapter. |
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Page 108
... range of k | is unchanged . Later , in connection with the heat capacity of solids , we shall need to know the frequency distribution of the normal modes , that is , the number of states per unit frequency range . In terms of the number ...
... range of k | is unchanged . Later , in connection with the heat capacity of solids , we shall need to know the frequency distribution of the normal modes , that is , the number of states per unit frequency range . In terms of the number ...
Page 251
... range of kT of such an electron are almost entirely filled , and it is generally not very probable that the electron will gain the 5kT≈ 0.1 ev necessary to excite it into an otherwise unoccupied state above the Fermi level . We can say ...
... range of kT of such an electron are almost entirely filled , and it is generally not very probable that the electron will gain the 5kT≈ 0.1 ev necessary to excite it into an otherwise unoccupied state above the Fermi level . We can say ...
Page 344
... range order . Consider a particular A atom : the probability23 that a particular nearest neigh- bor is a B atom is q ... range order , and as the temperature is lowered the long range 23 This estimate assumes that the probability is ...
... range order . Consider a particular A atom : the probability23 that a particular nearest neigh- bor is a B atom is q ... range order , and as the temperature is lowered the long range 23 This estimate assumes that the probability is ...
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