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 68
... example , has the form P 2a , + a2 + а3 . = 12 31 Another equally important example is the face - centered cubic ( fcc ) Bravais lattice . To construct the face - centered cubic Bravais lattice add to the simple cubic lattice of Figure ...
... example , has the form P 2a , + a2 + а3 . = 12 31 Another equally important example is the face - centered cubic ( fcc ) Bravais lattice . To construct the face - centered cubic Bravais lattice add to the simple cubic lattice of Figure ...
Page 112
... examples already described that Bravais lattices do fall naturally into categories on the basis of symmetries other than translational . Simple hexagonal Bravais lattices , for example , regardless of the c / a ratio , bear a closer ...
... examples already described that Bravais lattices do fall naturally into categories on the basis of symmetries other than translational . Simple hexagonal Bravais lattices , for example , regardless of the c / a ratio , bear a closer ...
Page 389
... example , lower and lower melting points ) . At the extreme right of the table are the column VIII elements , which afford the best example of molecular solids . The solid noble gases ( except for helium ) all crystallize in monatomic ...
... example , lower and lower melting points ) . At the extreme right of the table are the column VIII elements , which afford the best example of molecular solids . The solid noble gases ( except for helium ) all crystallize in monatomic ...
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