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 153
... equal for several different choices of K. If such degeneracy does not occur , then we have the expected class of free electron solutions : & = Ex - K , xx ek - K ) · r ̧ ( 9.5 ) If , however , there is a group of reciprocal lattice ...
... equal for several different choices of K. If such degeneracy does not occur , then we have the expected class of free electron solutions : & = Ex - K , xx ek - K ) · r ̧ ( 9.5 ) If , however , there is a group of reciprocal lattice ...
Page 276
... equal to half a wavelength ( Figure 14.7a ) can be accelerated ( or decelerated ) by the wave throughout their entire orbit , while electrons with orbit diameters equal to a whole wavelength ( Figure 14.7b ) must always be accelerated ...
... equal to half a wavelength ( Figure 14.7a ) can be accelerated ( or decelerated ) by the wave throughout their entire orbit , while electrons with orbit diameters equal to a whole wavelength ( Figure 14.7b ) must always be accelerated ...
Page 620
... ( equal numbers of positive and negative ion vacancies ) . ( c ) An ionic crystal with defects of the Frenkel type ( equal numbers of positive ion vacancies and interstitials ) . ( b ) + ( c ) of positive and negative ion vacancies ...
... ( equal numbers of positive and negative ion vacancies ) . ( c ) An ionic crystal with defects of the Frenkel type ( equal numbers of positive ion vacancies and interstitials ) . ( b ) + ( c ) of positive and negative ion vacancies ...
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