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 90
... lattice plane is defined to be any plane con- taining at least three noncollinear Bravais lattice points . Because of the translational symmetry of the ... lattice vector normal to the planes , for any. 90 Chapter 5 The Reciprocal Lattice.
... lattice plane is defined to be any plane con- taining at least three noncollinear Bravais lattice points . Because of the translational symmetry of the ... lattice vector normal to the planes , for any. 90 Chapter 5 The Reciprocal Lattice.
Page 91
... planes , for any wave vector shorter than K will give a plane wave with wavelength greater than 2π / K = d . Such a plane wave cannot have the same value on all ... plane with Miller indices h , k , I Miller Indices of Lattice Planes 91.
... planes , for any wave vector shorter than K will give a plane wave with wavelength greater than 2π / K = d . Such a plane wave cannot have the same value on all ... plane with Miller indices h , k , I Miller Indices of Lattice Planes 91.
Page 92
... lattice vector K = hb , kb2 + b3 , it will be contained in the continuous plane K r = A , for suitable choice of the constant A. This plane intersects the axes determined by the direct lattice primitive vectors a , at the points x1a1 ...
... lattice vector K = hb , kb2 + b3 , it will be contained in the continuous plane K r = A , for suitable choice of the constant A. This plane intersects the axes determined by the direct lattice primitive vectors a , at the points x1a1 ...
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