Introduction to Solid State Physics |
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Page 227
... Fermi - Dirac distribution function , and is plotted in Fig . 12.1 . To study the behavior of the function , we define an energy W such that F ( 12.20 ) α = -Wp / kT , giving ( 12.21 ) ƒ = F W is called FERMI - DIRAC DISTRIBUTION LAW 227.
... Fermi - Dirac distribution function , and is plotted in Fig . 12.1 . To study the behavior of the function , we define an energy W such that F ( 12.20 ) α = -Wp / kT , giving ( 12.21 ) ƒ = F W is called FERMI - DIRAC DISTRIBUTION LAW 227.
Page 239
... Fermi energy and u ( W ) is the velocity ( 2W / m ) corresponding to the Fermi 8 The derivation of this result is given by F. Seitz , Modern theory of solids , pp . 168-176 . It may be derived in an elementary way by recognizing that ...
... Fermi energy and u ( W ) is the velocity ( 2W / m ) corresponding to the Fermi 8 The derivation of this result is given by F. Seitz , Modern theory of solids , pp . 168-176 . It may be derived in an elementary way by recognizing that ...
Page 388
... Fermi - Dirac distribution , 224 , 227 , 229 Fermi energy , definition , 228 equation for , 229 , 231 intrinsic semiconductors , 276 table , 240 Fermi gas , pressure , 248 Fermi level , 371 Fermi temperature , 229 Ferrimagnetism ...
... Fermi - Dirac distribution , 224 , 227 , 229 Fermi energy , definition , 228 equation for , 229 , 231 intrinsic semiconductors , 276 table , 240 Fermi gas , pressure , 248 Fermi level , 371 Fermi temperature , 229 Ferrimagnetism ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali halides alkali metal alloy anisotropy antiferromagnetic approximation atoms axes axis Bardeen barium titanate boundary calculated charge coefficient conduction band cube Curie point Debye density diamagnetic dielectric constant diffraction diffusion dipole direction discussed dislocation displacement domains effect elastic electric field entropy equation equilibrium experimental F-center factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction interstitial ionic crystals ionized lattice constant lattice points London low temperatures magnetic field magnetic moment molecules motion nearest neighbor normal observed orbital p-n junctions parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium chloride potential Proc quantum range order region resonance result room temperature scattering Seitz semiconductor Shockley shown in Fig single crystal sodium chloride solids specimen spin superconducting susceptibility symmetry Table theory thermal tion unit volume valence values vector velocity wave functions x-ray zero