Solid State PhysicsThis book provides an introduction to the field of solid state physics for undergraduate students in physics, chemistry, engineering, and materials science. |
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Page 728
A description of the remarkable tunneling phenomena between superconductors
predicted by B. D. Josephson. CRITICAL TEMPERATURE The transition to the
superconducting state is a sharp one in bulk specimens. Above a critical ...
A description of the remarkable tunneling phenomena between superconductors
predicted by B. D. Josephson. CRITICAL TEMPERATURE The transition to the
superconducting state is a sharp one in bulk specimens. Above a critical ...
Page 733
Figure 34.4 (a) Magnetization curve of a type I superconductor. Below Hc no field
penetrates: B = 0 (or M = - H/4n). (See footnote 30 for the distinction between B
and H in a superconductor.) (b) Magnetization curve of a type II superconductor.
Figure 34.4 (a) Magnetization curve of a type I superconductor. Below Hc no field
penetrates: B = 0 (or M = - H/4n). (See footnote 30 for the distinction between B
and H in a superconductor.) (b) Magnetization curve of a type II superconductor.
Page 734
superconducting, and the field decays in a manner determined by the London
equation (see below). Circulating around each filament is a vortex of screening
current.20 Typical critical fields in type I superconductors are about 102 gauss
well ...
superconducting, and the field decays in a manner determined by the London
equation (see below). Circulating around each filament is a vortex of screening
current.20 Typical critical fields in type I superconductors are about 102 gauss
well ...
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Contents
The Drude Theory of Metals | 1 |
The Sommerfeld Theory of Metals | 29 |
Failures of the Free Electron Model | 57 |
Copyright | |
49 other sections not shown
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Solid State Physics: Advances in Research and Applications, Volume 42 Henry Ehrenreich Limited preview - 1989 |
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alkali atomic band structure Bloch boundary condition Bragg plane Bravais lattice Brillouin zone calculation carrier densities Chapter coefficients collisions conduction band conduction electrons contribution crystal momentum crystal structure density of levels dependence described determined direction Drude effect electric field electron gas electron-electron electronic levels energy gap equilibrium example face-centered cubic Fermi energy Fermi surface Figure free electron theory frequency given Hamiltonian hexagonal holes impurity independent electron approximation insulators integral interaction ionic crystals lattice planes lattice point linear magnetic field metals motion nearly free electron neutron normal modes Note number of electrons one-electron levels orbits periodic potential perpendicular phonon Phys plane waves primitive cell primitive vectors problem properties quantum reciprocal lattice vector region result scattering Schrodinger equation semiclassical semiclassical equations semiclassical model semiconductors simple cubic solid solution specific heat sphere spin superconducting symmetry temperature term thermal tight-binding valence vanishes velocity wave functions wave vector zero