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 320
... terms on the left side are often referred to as the drift terms , and the term on the right side as the collision term . When the form ( 16.8 ) is used for the collision term , the Boltzmann equation in general becomes a nonlinear ...
... terms on the left side are often referred to as the drift terms , and the term on the right side as the collision term . When the form ( 16.8 ) is used for the collision term , the Boltzmann equation in general becomes a nonlinear ...
Page 648
... term that is linear in H vanishes identically ( as it sometimes does ) , it will almost always be the dominant term even when the field is very strong ( ~ 104 gauss ) . If it does not vanish , < n | ( L2 + g。S2 ) | n ) will be of order ...
... term that is linear in H vanishes identically ( as it sometimes does ) , it will almost always be the dominant term even when the field is very strong ( ~ 104 gauss ) . If it does not vanish , < n | ( L2 + g。S2 ) | n ) will be of order ...
Page 766
... term on the right of ( E.8 ) comes from placing the second - order term in H + q ( Eq . ( E.2 ) ) into the first - order term in the perturbation theory formula ( Eq . ( E.4 ) ) . The second term on the right comes from placing the ...
... term on the right of ( E.8 ) comes from placing the second - order term in H + q ( Eq . ( E.2 ) ) into the first - order term in the perturbation theory formula ( Eq . ( E.4 ) ) . The second term on the right comes from placing the ...
Contents
The Drude Theory of Metals | 1 |
The Sommerfeld Theory of Metals | 29 |
Failures of the Free Electron Model | 57 |
Copyright | |
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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 density of levels dependence described determined Drude effect electric field electron gas electron-electron electronic levels energy gap equilibrium example Fermi energy Fermi surface Figure frequency given Hamiltonian hexagonal holes impurity independent electron approximation insulators integral interaction ionic crystals k-space k₂ 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 Schrödinger equation semiclassical semiclassical equations semiclassical model semiconductors simple cubic solid solution specific heat sphere spin superconducting symmetry temperature term thermal tight-binding valence valence band vanishes velocity wave functions wave vector zero