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 86
... satisfying eik R = 1 ( 5.1 ) we can charac- ( 5.2 ) for all R in the Bravais lattice . Note that a reciprocal lattice ... satisfy ( 5.2 ) , so , obviously , will their sum and difference . It is worth considering a more clumsy proof of ...
... satisfying eik R = 1 ( 5.1 ) we can charac- ( 5.2 ) for all R in the Bravais lattice . Note that a reciprocal lattice ... satisfy ( 5.2 ) , so , obviously , will their sum and difference . It is worth considering a more clumsy proof of ...
Page 178
... satisfies the atomic Schrödinger equation ( 10.1 ) , then it will also satisfy the crystal Schrödinger equation ( 10.2 ) , provided that AU ( r ) vanishes wherever ( r ) does not . If this were indeed the case , then each atomic level ...
... satisfies the atomic Schrödinger equation ( 10.1 ) , then it will also satisfy the crystal Schrödinger equation ( 10.2 ) , provided that AU ( r ) vanishes wherever ( r ) does not . If this were indeed the case , then each atomic level ...
Page 201
... satisfy the atomic Schrödinger equation : 3 . k , & ħ2 - V2ke ( r ) + V ( r R ) ke ( r ) = && ( r ) , │r – R│ < 0 ... satisfies not ( 11.15 ) but HOKE = ( h2k2 / 2m ) . Note also that , in general , e will have a discontinuous ...
... satisfy the atomic Schrödinger equation : 3 . k , & ħ2 - V2ke ( r ) + V ( r R ) ke ( r ) = && ( r ) , │r – R│ < 0 ... satisfies not ( 11.15 ) but HOKE = ( h2k2 / 2m ) . Note also that , in general , e will have a discontinuous ...
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