## 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

(4.3) Figure 4.6 Three primitive vectors, specified in Eq. (4.3), for the body-

centered cubic Bravais lattice. The lattice is formed by taking all linear

combinations of the primitive vectors with integral coefficients. The point P, for

(4.3) Figure 4.6 Three primitive vectors, specified in Eq. (4.3), for the body-

centered cubic Bravais lattice. The lattice is formed by taking all linear

combinations of the primitive vectors with integral coefficients. The point P, for

**example**, is P = -a, ...Page 112

For

only on the existence of three primitive direct lattice vectors af, and not on any

special relations that may hold among them.1 The translational symmetries are

by ...

For

**example**, the existence and basic properties of the reciprocal lattice dependonly on the existence of three primitive direct lattice vectors af, and not on any

special relations that may hold among them.1 The translational symmetries are

by ...

Page 684

The Hartree-Fock approximation is improved if one lets the electrons screen the

exchange interaction (page 344), and thereby reduce its spatial range. This

improvement alters the Hartree-Fock prediction quite drastically. For

the ...

The Hartree-Fock approximation is improved if one lets the electrons screen the

exchange interaction (page 344), and thereby reduce its spatial range. This

improvement alters the Hartree-Fock prediction quite drastically. For

**example**, inthe ...

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### Contents

The Drude Theory of Metals | 1 |

Failures of the Free Electron Model | 57 |

The facecentered cubic elements | 72 |

Copyright | |

34 other sections not shown

### Other editions - View all

Solid State Physics: Advances in Research and Applications, Volume 42 Henry Ehrenreich Limited preview - 1989 |

### 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 crystal structure density of levels dependence described determined direction Drude effect electric field electron gas electron-electron electronic levels energy gap equilibrium example Fermi energy Fermi surface Figure free electron theory frequency given Hamiltonian hexagonal holes impurity independent electron approximation insulators integral interaction ionic crystals lattice planes 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 Schrodinger equation semiclassical semiclassical equations semiclassical model semiconductors simple cubic solid solution specific heat sphere spin superconducting symmetry temperature term thermal tight-binding valence vanishes velocity wave functions wave vector zero