Introduction to Solid State PhysicsProblems after each chapter. |
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Page 235
... equilibrium at temperature T. In the absence of an applied electric field the average or drift velocity , N ( 10.1 ) VD = Vi , N will be zero , as in equilibrium there are just as many electrons moving in one direction as in the ...
... equilibrium at temperature T. In the absence of an applied electric field the average or drift velocity , N ( 10.1 ) VD = Vi , N will be zero , as in equilibrium there are just as many electrons moving in one direction as in the ...
Page 236
... equilibrium distribu- tion , the approach to equilibrium is described by the appropriate solu- tion of ( 10.3 ) : ( 10.4 ) VD ( 1 ) = ▽ D ( 0 ) e ̄t / . We have thus arranged things so that a disturbance from equilibrium dies out ...
... equilibrium distribu- tion , the approach to equilibrium is described by the appropriate solu- tion of ( 10.3 ) : ( 10.4 ) VD ( 1 ) = ▽ D ( 0 ) e ̄t / . We have thus arranged things so that a disturbance from equilibrium dies out ...
Page 591
... equilibrium dF = dF = dn + μι dn . 0 , whence we have the stated result μ ; = μια This result has an important application to contact potential problems , for it tells us that in equilibrium the Fermi level must have a constant value in ...
... equilibrium dF = dF = dn + μι dn . 0 , whence we have the stated result μ ; = μια This result has an important application to contact potential problems , for it tells us that in equilibrium the Fermi level must have a constant value in ...
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