Introduction to Solid State Physics |
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Page 420
... applied magnetic field B. At a temperature T < Te the metal is a super- conductor in zero magnetic field , so that Fs ( T , O ) is lower than Fx ( T , 0 ) . An applied magnetic field increases Fs by Ba2 / 877 , in CGS units , so that ...
... applied magnetic field B. At a temperature T < Te the metal is a super- conductor in zero magnetic field , so that Fs ( T , O ) is lower than Fx ( T , 0 ) . An applied magnetic field increases Fs by Ba2 / 877 , in CGS units , so that ...
Page 436
... applied mag- netic field is increased . A superconductor is type I if the surface energy is always positive , and type II if the surface energy becomes negative as the mag- netic field is increased . To refer to Fig . 6b , the surface ...
... applied mag- netic field is increased . A superconductor is type I if the surface energy is always positive , and type II if the surface energy becomes negative as the mag- netic field is increased . To refer to Fig . 6b , the surface ...
Page 500
... applied magnetic field . In electromagnetism we are familiar with Lenz's law : when the flux through an electrical ... field is present . The magnetic field produced by the induced current is opposite to the applied field , and the ...
... applied magnetic field . In electromagnetism we are familiar with Lenz's law : when the flux through an electrical ... field is present . The magnetic field produced by the induced current is opposite to the applied field , and the ...
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