Introduction to Solid State PhysicsProblems after each chapter. |
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Page 150
... resistivity W of a fairly pure metal at low tem- peratures ( T < / 10 ) may be written in the form ( 6.57 ) 1 W = Wo + W ; Wi 0 - K i Here Wo is the thermal resistivity due to electron scattering by lattice vibrations and W ; is the ...
... resistivity W of a fairly pure metal at low tem- peratures ( T < / 10 ) may be written in the form ( 6.57 ) 1 W = Wo + W ; Wi 0 - K i Here Wo is the thermal resistivity due to electron scattering by lattice vibrations and W ; is the ...
Page 239
... resistivity measurements of Cu and Ag films at room temperature , shown with curves calculated from theory to obtain approximate values of mean free paths . Here p ' is the resistivity in the film ; p is the bulk resistivity ...
... resistivity measurements of Cu and Ag films at room temperature , shown with curves calculated from theory to obtain approximate values of mean free paths . Here p ' is the resistivity in the film ; p is the bulk resistivity ...
Page 305
... resistivity of a metal containing impurity atoms may usually be written in the form ( 11.92 ) PL p = Pi + PL , where p is the resistivity caused by thermal motion of the lattice , and p ; is the resistivity caused by scattering of the ...
... resistivity of a metal containing impurity atoms may usually be written in the form ( 11.92 ) PL p = Pi + PL , where p is the resistivity caused by thermal motion of the lattice , and p ; is the resistivity caused by scattering of the ...
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