Introduction to Solid State PhysicsProblems after each chapter. |
From inside the book
Results 1-3 of 76
Page 262
... DISTRIBUTION ON THE ELECTRICAL CONDUCTIVITY It is a somewhat surprising fact that the introduction of the Fermi- Dirac distribution in place of the classical Maxwell - Boltzmann dis- tribution usually has little influence on the ...
... DISTRIBUTION ON THE ELECTRICAL CONDUCTIVITY It is a somewhat surprising fact that the introduction of the Fermi- Dirac distribution in place of the classical Maxwell - Boltzmann dis- tribution usually has little influence on the ...
Page 263
... distribution . ( b ) Distribution shifted by electric field applied for ( c ) Difference between steady - state distribution and equilibrium distribution . time T. the steady - state distribution , = P ( Vr , T ) P ( vr , 0 ) ( eEr / m ) ...
... distribution . ( b ) Distribution shifted by electric field applied for ( c ) Difference between steady - state distribution and equilibrium distribution . time T. the steady - state distribution , = P ( Vr , T ) P ( vr , 0 ) ( eEr / m ) ...
Page 264
... distribution . ( b ) Distribution shifted by electric field applied for time 7 . ( c ) Difference between steady - state distribution and equilibrium distribution . response of the distribution to the electric field , because each ...
... distribution . ( b ) Distribution shifted by electric field applied for time 7 . ( c ) Difference between steady - state distribution and equilibrium distribution . response of the distribution to the electric field , because each ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
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 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