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 12
... ( known today as the Hall voltage ) , which Hall was able to observe . Hall's experiment is depicted in Figure 1.3 . An electric field E is applied to a wire extending in the x - direction and a current density j , flows in the wire . In ...
... ( known today as the Hall voltage ) , which Hall was able to observe . Hall's experiment is depicted in Figure 1.3 . An electric field E is applied to a wire extending in the x - direction and a current density j , flows in the wire . In ...
Page 142
... known as an intrinsic semiconductor ( Chapter 28 ) . Because the number of levels in a Some levels band is equal to ... known as the Fermi surface , and is the generalization to Bloch electrons of the free electron Fermi sphere . The ...
... known as an intrinsic semiconductor ( Chapter 28 ) . Because the number of levels in a Some levels band is equal to ... known as the Fermi surface , and is the generalization to Bloch electrons of the free electron Fermi sphere . The ...
Page 331
... known as the Hartree equations . These nonlinear equations for the one - electron wave functions and energies are solved , in practice , by iteration : A form is guessed for Uel ( the term in brackets in ( 17.7 ) ) on the basis of which ...
... known as the Hartree equations . These nonlinear equations for the one - electron wave functions and energies are solved , in practice , by iteration : A form is guessed for Uel ( the term in brackets in ( 17.7 ) ) on the basis of which ...
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