Introduction to Solid State Physics |
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Page 46
... applied . Thus the stress component X2 represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the x direction ; the stress com- ponent X , represents a force applied in the x direction to a unit ...
... applied . Thus the stress component X2 represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the x direction ; the stress com- ponent X , represents a force applied in the x direction to a unit ...
Page 89
... applied electric field ( Fig . 6.1 ) . The field Eloc at any atom may be written as a sum ( 6.1 ) = Eloc E0 + E1 + E2 + E3 , 1 where Eo is the electric field applied from external sources ; E1 is the " depolarization field " resulting ...
... applied electric field ( Fig . 6.1 ) . The field Eloc at any atom may be written as a sum ( 6.1 ) = Eloc E0 + E1 + E2 + E3 , 1 where Eo is the electric field applied from external sources ; E1 is the " depolarization field " resulting ...
Page 91
Charles Kittel. principal axes parallel to the applied field , the polarization will be parallel to the applied field , as will the depolarization field E1 , which it is found may be calculated from the polarization P by a relation of ...
Charles Kittel. principal axes parallel to the applied field , the polarization will be parallel to the applied field , as will the depolarization field E1 , which it is found may be calculated from the polarization P by a relation of ...
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