## Solid state physics |

### From inside the book

Results 1-3 of 75

Page 226

This is because, given the values of k and r at t = 0, the semiclassical equations,

being six first-order equations in six variables, uniquely

subsequent (and all prior) times, just as in ordinary classical mechanics the ...

This is because, given the values of k and r at t = 0, the semiclassical equations,

being six first-order equations in six variables, uniquely

**determine**k and r at allsubsequent (and all prior) times, just as in ordinary classical mechanics the ...

Page 264

We have already encountered one such quantity, the high-field Hall constant,

which (in uncompensated metals with no open orbits for the given field direction)

is entirely

We have already encountered one such quantity, the high-field Hall constant,

which (in uncompensated metals with no open orbits for the given field direction)

is entirely

**determined**by the /c-space volume enclosed by the hole-like and ...Page 354

In limiting ourselves to bulk properties we are neglecting the increasingly

important field of surface physics, which deals with phenomena such as catalysis

or crystal growth, which are entirely

atoms with ...

In limiting ourselves to bulk properties we are neglecting the increasingly

important field of surface physics, which deals with phenomena such as catalysis

or crystal growth, which are entirely

**determined**by the interaction of surfaceatoms with ...

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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