Introduction to Solid State Physics |
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Page 51
... solution is given by a longitudinal wave , u = uoei ( wi ― kx ) , moving along the x cube edge ; from ( 3.25 ) so that the velocity is ( 3.26 ) -w2p - k2c11 , = v = w / k = ( C11 / p ) . Another solution is given by a transverse or ...
... solution is given by a longitudinal wave , u = uoei ( wi ― kx ) , moving along the x cube edge ; from ( 3.25 ) so that the velocity is ( 3.26 ) -w2p - k2c11 , = v = w / k = ( C11 / p ) . Another solution is given by a transverse or ...
Page 64
... solution for kπ / L has uα sin nra / L and vanishes for n = 0 and n = N as required , with a maximum for n = N / 2 . The solution for k NT / LT / α = km has u ∞ sin na , permitting no motion at all , because sin na vanishes at each ...
... solution for kπ / L has uα sin nra / L and vanishes for n = 0 and n = N as required , with a maximum for n = N / 2 . The solution for k NT / LT / α = km has u ∞ sin na , permitting no motion at all , because sin na vanishes at each ...
Page 213
... solution H = Ho . If we include the displacement current we have ( 11.24 ) Ac ? 4π AC2 [ V3H - # ] - 1 H. H Equations ( 11.17 ) and ( 11.22 ) , when applied to the superconducting electrons , are known as the London equations and are ...
... solution H = Ho . If we include the displacement current we have ( 11.24 ) Ac ? 4π AC2 [ V3H - # ] - 1 H. H Equations ( 11.17 ) and ( 11.22 ) , when applied to the superconducting electrons , are known as the London equations and are ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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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