Solid State PhysicsThis book provides an introduction to the field of solid state physics for undergraduate students in physics, chemistry, engineering, and materials science. |
From inside the book
Results 1-3 of 89
Page 72
... cell , the volume of a primitive cell is independent of the choice of cell . It also follows from the definition of a primitive cell that , given any two primitive cells of arbitrary shape , it is possible to cut the first up into ...
... cell , the volume of a primitive cell is independent of the choice of cell . It also follows from the definition of a primitive cell that , given any two primitive cells of arbitrary shape , it is possible to cut the first up into ...
Page 73
Neil W. Ashcroft, N. David Mermin. UNIT CELL ; CONVENTIONAL UNIT CELL One can fill space up with nonprimitive unit cells ( known simply as unit cells or conventional unit cells ) . A unit cell is a region that just fills space without ...
Neil W. Ashcroft, N. David Mermin. UNIT CELL ; CONVENTIONAL UNIT CELL One can fill space up with nonprimitive unit cells ( known simply as unit cells or conventional unit cells ) . A unit cell is a region that just fills space without ...
Page 74
... cell is a primitive cell . Since there is nothing in the definition of the Wigner - Seitz cell that refers to any particular choice of primitive vectors , the Wigner - Seitz cell will be as symmetrical as the Bravais lattice.12 The ...
... cell is a primitive cell . Since there is nothing in the definition of the Wigner - Seitz cell that refers to any particular choice of primitive vectors , the Wigner - Seitz cell will be as symmetrical as the Bravais lattice.12 The ...
Contents
The Drude Theory of Metals | 1 |
The Sommerfeld Theory of Metals | 29 |
Failures of the Free Electron Model | 57 |
Copyright | |
48 other sections not shown
Other editions - View all
Common terms and phrases
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