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 70
Page 412
... correction is strictly linear in h , then the correction to the energy must have the form Au = e ^ ƒ ( r / o ) , where ƒ depends on the particular noble gas in question only through the ratio r / σ , and ( 20.29 ) Λ = h σν Με ( 20.30 ) ...
... correction is strictly linear in h , then the correction to the energy must have the form Au = e ^ ƒ ( r / o ) , where ƒ depends on the particular noble gas in question only through the ratio r / σ , and ( 20.29 ) Λ = h σν Με ( 20.30 ) ...
Page 530
... correction to the electronic specific heat ( Eq . ( 2.102 ) , evaluated in the free electron approximation ) by a factor 1 3M Z Z1 / 3 m 3/2 ( 26.55 ) 3. Phonon Corrections to the Electronic Energy In the limit op → O , the correction ...
... correction to the electronic specific heat ( Eq . ( 2.102 ) , evaluated in the free electron approximation ) by a factor 1 3M Z Z1 / 3 m 3/2 ( 26.55 ) 3. Phonon Corrections to the Electronic Energy In the limit op → O , the correction ...
Page 664
... correction is tied to the Fermi level , it has very little effect on the magnetization as the field varies , leading to a correction factor in the susceptibility that is only of order ( m / M ) 12 ( in contrast to the correction of ...
... correction is tied to the Fermi level , it has very little effect on the magnetization as the field varies , leading to a correction factor in the susceptibility that is only of order ( m / M ) 12 ( in contrast to the correction of ...
Contents
The Drude Theory of Metals | 1 |
Failures of the Free Electron Model | 57 |
Crystal Lattices | 63 |
Copyright | |
19 other sections not shown
Other editions - View all
Common terms and phrases
alkali atomic band structure Bloch Bragg plane Bravais lattice Brillouin zone calculation carrier densities Chapter charge density coefficients collision conduction band conduction electrons contribution crystal momentum crystal structure density of levels dependence depletion layer described dielectric constant direction distribution Drude Drude model effect electric field electron gas electron-electron electronic levels electrostatic energy gap example Fermi energy Fermi surface Figure free electron frequency given Hamiltonian hexagonal holes impurity independent electron approximation insulators interaction ionic crystals k-space lattice planes lattice point linear low temperatures macroscopic magnetic field metals neutron normal modes number of electrons one-electron levels orbits periodic potential perpendicular phonon Phys positive primitive cell primitive vectors Problem properties quantum reciprocal lattice vector region result scattering Schrödinger equation semiclassical semiconductors simple cubic solid solution specific heat spin superconducting symmetry term theory valence band vanishes velocity wave functions wave vector zero