## Solid state physics |

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Results 1-3 of 77

Page 61

Of the difficulties

law at intermediate temperatures (Id) has a resolution that requires abandoning

the relaxation time approximation even at the most gross qualitative level of ...

Of the difficulties

**described**previously, only the problem of the Wiedemann-Franzlaw at intermediate temperatures (Id) has a resolution that requires abandoning

the relaxation time approximation even at the most gross qualitative level of ...

Page 112

In Chapters 4 and 5, only the translational symmetries of Bravais lattices were

reciprocal lattice depend only on the existence of three primitive direct lattice ...

In Chapters 4 and 5, only the translational symmetries of Bravais lattices were

**described**and exploited. For example, the existence and basic properties of thereciprocal lattice depend only on the existence of three primitive direct lattice ...

Page 128

... three mutually perpendicular primitive vectors are a, b, and c. The structure of

rhombic sulfur is complex, with 128 atoms per unit cell. The others can be

Wyckoff.

... three mutually perpendicular primitive vectors are a, b, and c. The structure of

rhombic sulfur is complex, with 128 atoms per unit cell. The others can be

**described**in terms of an eight-atom unit cell. For details the reader is referred toWyckoff.

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### Contents

The Dmle 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

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 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 ions 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 valence band vanishes velocity wave functions wave vector zero