Introduction to Solid State Physics |
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Page 435
... superconducting electrons , known as Josephson tunneling . Type II Superconductors There is no difference in the ... superconducting . At a much higher field , sometimes 100 kG or more , the flux penetrates completely and all supercon ...
... superconducting electrons , known as Josephson tunneling . Type II Superconductors There is no difference in the ... superconducting . At a much higher field , sometimes 100 kG or more , the flux penetrates completely and all supercon ...
Page 436
... superconductor when both superconducting and normal states coexist . Slabs in one state are intercalated between slabs of the other state . Because the interface energy is positive , the electronic energy would be lowered if the ...
... superconductor when both superconducting and normal states coexist . Slabs in one state are intercalated between slabs of the other state . Because the interface energy is positive , the electronic energy would be lowered if the ...
Page 444
... superconductors , I and II . In a bulk specimen of type I superconductor the superconducting state is destroyed and the normal state is restored by application of an external magnetic field in excess of a critical value Hc . A type II ...
... superconductors , I and II . In a bulk specimen of type I superconductor the superconducting state is destroyed and the normal state is restored by application of an external magnetic field in excess of a critical value Hc . A type II ...
Contents
CRYSTAL STRUCTURE | 1 |
CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |
CRYSTAL BINDING | 95 |
Copyright | |
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absolute zero absorption alkali halide alloy antiferromagnet applied field atoms axis boundary Brillouin zone calculated Chapter charge components conduction band conduction electrons crystal structure cubic density dielectric constant dielectric function diffraction dipole direction dislocation dispersion relation effective mass elastic electric field electron concentration electron gas energy gap equation equilibrium excited exciton experimental F center Fermi surface ferroelectric ferromagnetic Figure free electron frequency function given heat capacity hole impurity interaction ionic lattice constant lattice points low temperatures magnetic field magnetic moment magnon metal modes momentum motion nearest neighbors neutron normal nuclear optical orbital paramagnetic particle phase phonon Phys plane polarization positive potential primitive cell quantum reciprocal lattice vector region resonance result room temperature scattering semiconductor shown in Fig space specimen sphere superconducting theory thermal tion transition unit vacancy valence band velocity wavefunction wavelength wavevector x-ray