Introduction to Solid State PhysicsProblems after each chapter. |
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Page 454
... superconducting state . Intermediate state . The magnetization curve for a sphere in the superconducting state ( Fig . 16.4 ) shows that superconductivity is partially destroyed for H. < H < He . This region is called the intermediate ...
... superconducting state . Intermediate state . The magnetization curve for a sphere in the superconducting state ( Fig . 16.4 ) shows that superconductivity is partially destroyed for H. < H < He . This region is called the intermediate ...
Page 471
... superconducting material will then become something like a prolate spheroid , thereby reducing the field in the interior . The material at the boundary between nor- mal and superconducting regions will naturally be in the field He , but ...
... superconducting material will then become something like a prolate spheroid , thereby reducing the field in the interior . The material at the boundary between nor- mal and superconducting regions will naturally be in the field He , but ...
Page 475
... superconducting ) np = 0.14 X 106 , while for lead ( which is superconducting ) np = 3.1 X 10. In fact , the theory is probably not as good as the extent of the agreement with the above criterion . Bardeen 35 has given a discussion of ...
... superconducting ) np = 0.14 X 106 , while for lead ( which is superconducting ) np = 3.1 X 10. In fact , the theory is probably not as good as the extent of the agreement with the above criterion . Bardeen 35 has given a discussion of ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 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 levels 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 region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero