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 346
... requires that these two electrons can only scatter into unoccupied levels , whose energies & 3 and 84 must therefore be greater than & F . Thus we require that E2 < EF , E3 > EF , E4 > EF . In addition , energy conservation requires ...
... requires that these two electrons can only scatter into unoccupied levels , whose energies & 3 and 84 must therefore be greater than & F . Thus we require that E2 < EF , E3 > EF , E4 > EF . In addition , energy conservation requires ...
Page 432
... requires k to have the form : k = 2π η a N n an integer . ( 22.27 ) Note that if k is changed by 2л / a , the ... requiring k to lie in the first Brillouin zone ( Chapter 8 ) . Although there are 2N solutions , there are only N “ normal ...
... requires k to have the form : k = 2π η a N n an integer . ( 22.27 ) Note that if k is changed by 2л / a , the ... requiring k to lie in the first Brillouin zone ( Chapter 8 ) . Although there are 2N solutions , there are only N “ normal ...
Page 556
... requires very little applied field to alter substantially the displacement polarization of the crystal . Dielectric constants as large as 105 have been observed near ferroelectric transition points . In an ideal experiment the ...
... requires very little applied field to alter substantially the displacement polarization of the crystal . Dielectric constants as large as 105 have been observed near ferroelectric transition points . In an ideal experiment the ...
Contents
The Drude Theory of Metals | 1 |
Failures of the Free Electron Model | 57 |
Crystal Lattices | 63 |
Copyright | |
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alkali atomic band structure Bloch Bragg plane Bravais lattice Brillouin zone calculation carrier densities Chapter charge density coefficients collision conduction band conduction electrons contribution crystal momentum crystal structure density of levels dependence depletion layer described dielectric constant direction distribution Drude Drude model effect electric field electron gas electron-electron electronic levels electrostatic energy gap example Fermi energy Fermi surface Figure free electron frequency given Hamiltonian hexagonal holes impurity independent electron approximation insulators interaction ionic crystals k-space lattice planes lattice point linear low temperatures macroscopic magnetic field metals neutron normal modes number of electrons one-electron levels orbits periodic potential perpendicular phonon Phys positive primitive cell primitive vectors Problem properties quantum reciprocal lattice vector region result scattering Schrödinger equation semiclassical semiconductors simple cubic solid solution specific heat spin superconducting symmetry term theory valence band vanishes velocity wave functions wave vector zero