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 71
Page 139
Note , however , that although the free electron wave vector is simply p / h , where p is the momentum of the electron , in the Bloch case k is not proportional to the electronic momentum . This is clear on general grounds , since the ...
Note , however , that although the free electron wave vector is simply p / h , where p is the momentum of the electron , in the Bloch case k is not proportional to the electronic momentum . This is clear on general grounds , since the ...
Page 472
We emphasize , however , that the crystal momentum of a phonon is not , in general , accompanied by any real momentum of the ionic system . " Crystal momentum " is simply a name for ħ times the phonon wave vector .
We emphasize , however , that the crystal momentum of a phonon is not , in general , accompanied by any real momentum of the ionic system . " Crystal momentum " is simply a name for ħ times the phonon wave vector .
Page 788
Scattering of a Neutron by an Insulator Suppose that at the start of the experiment the crystal is in an eigenstate of the harmonic Hamiltonian with phonon occupation numbers nk , and the neutron is in a state with real momentum p ...
Scattering of a Neutron by an Insulator Suppose that at the start of the experiment the crystal is in an eigenstate of the harmonic Hamiltonian with phonon occupation numbers nk , and the neutron is in a state with real momentum p ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
The Drude Theory of Metals | 1 |
Failures of the Free Electron Model | 57 |
Crystal Lattices | 63 |
Copyright | |
20 other sections not shown
Other editions - View all
Common terms and phrases
additional applied approximation assume atomic band Bragg Bravais lattice calculation carrier Chapter charge close collision compared condition conduction consider constant containing contribution correction crystal cubic density dependence described determined direction discussion distance distribution effect elements energy equation equilibrium example fact factor Fermi surface field Figure follows free electron frequency function give given hexagonal holes important impurity independent integral interaction ionic ions known lattice vector leading levels limit linear magnetic field mean measured metals mode momentum normal Note observed orbits periodic phonon plane positive possible potential present primitive cell Problem properties reciprocal lattice reflection region relation requires result satisfy scattering Show simple single solid solution space specific heat structure surface symmetry Table temperature term theory thermal unit vanishes volume wave functions wave vector zero zone