Introduction to Solid State Physics |
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Page 74
... condition that the number of states considered should come out equal to N L / a . Now km π / a as before , so that wm vokmπvo / a . = = = πυο / α . In Fig . 5.1 we compare the results given by Blackman1 for the heat capacities as ...
... condition that the number of states considered should come out equal to N L / a . Now km π / a as before , so that wm vokmπvo / a . = = = πυο / α . In Fig . 5.1 we compare the results given by Blackman1 for the heat capacities as ...
Page 310
Charles Kittel. exp ( -eEx / kT ) . The condition that in equilibrium no net current should flow is ( 15.22 ) une - D ... CONDITIONS AND THE RECIPROCAL LATTICE1 The conditions 310 IMPERFECTIONS IN SOLIDS : I.
Charles Kittel. exp ( -eEx / kT ) . The condition that in equilibrium no net current should flow is ( 15.22 ) une - D ... CONDITIONS AND THE RECIPROCAL LATTICE1 The conditions 310 IMPERFECTIONS IN SOLIDS : I.
Page 352
... condition hwij >> kT ; that is , only the ground state i is significantly populated at the temperature considered . D. ONSAGER THEORY OF THE DIELECTRIC CONSTANT OF POLAR SUBSTANCES The Lorentz treatment of the local field assumes ...
... condition hwij >> kT ; that is , only the ground state i is significantly populated at the temperature considered . D. ONSAGER THEORY OF THE DIELECTRIC CONSTANT OF POLAR SUBSTANCES The Lorentz treatment of the local field assumes ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali alloy anisotropy antiferromagnetic approximately 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 energy entropy equation equilibrium experimental F-centers factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction ionic crystals ionized ions lattice constant lattice points London low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed optical orbital parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium potassium chloride potential Proc quantum resonance result room temperature scattering Seitz shear Shockley shown in Fig single crystal sodium chloride solids specimen spin strain stress superconducting surface susceptibility symmetry Table theory thermal tion transition unit volume vacancy valence values vector velocity wave functions x-ray zero