Introduction to Solid State PhysicsProblems after each chapter. |
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Page 456
... superconducting state to the normal state . That is , the superconducting state is more ordered than the normal state . The difference in entropy is of the order of 10-3 R per mole , instead of the order of R as in an ordinary ...
... superconducting state to the normal state . That is , the superconducting state is more ordered than the normal state . The difference in entropy is of the order of 10-3 R per mole , instead of the order of R as in an ordinary ...
Page 459
... superconductors . ( b ) The ferromagnetic and antiferromagnetic metals are not super- conductors . ( c ) Superconducting metals are not as good conductors at room temperature as the normal metals at room temperature . For exam- ple ...
... superconductors . ( b ) The ferromagnetic and antiferromagnetic metals are not super- conductors . ( c ) Superconducting metals are not as good conductors at room temperature as the normal metals at room temperature . For exam- ple ...
Page 475
... superconducting ) np = 0.14 × 106 , while for lead ( which is superconducting ) np 3.1 X 106 . = Note added in third printing : Bardeen , Cooper , and Schrieffer 35 have developed a remarkable theory which accounts in considerable ...
... superconducting ) np = 0.14 × 106 , while for lead ( which is superconducting ) np 3.1 X 106 . = Note added in third printing : Bardeen , Cooper , and Schrieffer 35 have developed a remarkable theory which accounts in considerable ...
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 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