Introduction to Solid State PhysicsProblems after each chapter. |
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Page 199
... transition , but is rather accompanied by a discontinuity in the heat capacity ; such a transition is known in thermodynamics as a second order transition ; a case B transition is DIELECTRIC CONSTANTS NEAR THE CURIE POINT 199.
... transition , but is rather accompanied by a discontinuity in the heat capacity ; such a transition is known in thermodynamics as a second order transition ; a case B transition is DIELECTRIC CONSTANTS NEAR THE CURIE POINT 199.
Page 459
... transition temperature , high critical field , incomplete Meissner effect , breakdown of Silsbee's rule , and a broad transition region ; because of these properties they are known as non - ideal or hard superconductors . The anomalous ...
... transition temperature , high critical field , incomplete Meissner effect , breakdown of Silsbee's rule , and a broad transition region ; because of these properties they are known as non - ideal or hard superconductors . The anomalous ...
Page 462
... TRANSITION It has been demonstrated experimentally by van Laer and Keesom " that the transition between the normal and superconducting states is thermodynamically reversible , in the same sense that with slow evapo- ration the transition ...
... TRANSITION It has been demonstrated experimentally by van Laer and Keesom " that the transition between the normal and superconducting states is thermodynamically reversible , in the same sense that with slow evapo- ration the transition ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS 85 | 85 |
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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 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