## Solid state physics |

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Page 258

OTHER THERMOELECTRIC

the Peltier

OTHER THERMOELECTRIC

**EFFECTS**There is a variety of other thermoelectric**effects**. The Thomson**effect**is described in Problem 5, and we mention here onlythe Peltier

**effect**.41 If an electric current is driven in a bimetallic circuit that is ...Page 265

Similar oscillatory behavior has been observed not only in the susceptibility, but

also in the conductivity (Shubnikov-de Haas

dependence of sample size on magnetic field strength), and, when measured

with ...

Similar oscillatory behavior has been observed not only in the susceptibility, but

also in the conductivity (Shubnikov-de Haas

**effect**), the magnetostriction (dependence of sample size on magnetic field strength), and, when measured

with ...

Page 277

One no longer examines a resonant

attenuation assuming that it is entirely due to ... near as simple as either the

extremal areas furnished by the de Haas-van Alphen

diameters one ...

One no longer examines a resonant

**effect**, but simply calculates the rate ofattenuation assuming that it is entirely due to ... near as simple as either the

extremal areas furnished by the de Haas-van Alphen

**effect**or the extremaldiameters one ...

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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

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### 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