## Solid state physics |

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Page 219

Crystal Momentum Is Not Momentum Note that within each band the equations of

motion (12.6) are the same as the ... which we state here without proof.13 At a

given point in k-space the

the ...

Crystal Momentum Is Not Momentum Note that within each band the equations of

motion (12.6) are the same as the ... which we state here without proof.13 At a

given point in k-space the

**semiclassical equations**will be valid for electrons inthe ...

Page 221

The dissatisfied reader is referred to Appendix H for a further way of rendering

the

written in a very compact Hamiltonian form. To find a really compelling set of ...

The dissatisfied reader is referred to Appendix H for a further way of rendering

the

**semiclassical equations**more plausible. There it is shown that they can bewritten in a very compact Hamiltonian form. To find a really compelling set of ...

Page 222

The

at all times, even in the presence of space- and time-dependent electric and

magnetic fields. This is a direct consequence of the semiclassical analogue of ...

The

**semiclassical equations**(12.6) imply that a filled band remains a filled bandat all times, even in the presence of space- and time-dependent electric and

magnetic fields. This is a direct consequence of the semiclassical analogue of ...

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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