## 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 356

Now consider a finite

configuration by simply occupying some finite region V of the Bravais lattice

occupied in the infinite

density in ...

Now consider a finite

**crystal**. Suppose that we could represent the ionicconfiguration by simply occupying some finite region V of the Bravais lattice

occupied in the infinite

**crystal**. Suppose , furthermore , that the electronic chargedensity in ...

Page 358

2 ( a ) The actual form of the electric charge density near the surface of a

neglecting possible slight displacements of the ions near the surface from their

sites in the infinite

2 ( a ) The actual form of the electric charge density near the surface of a

**crystal**(neglecting possible slight displacements of the ions near the surface from their

sites in the infinite

**crystal**) . Note the electron deficiency in the two cells nearest ...Page 555

26

are called pyroelectric . 27 In equilibrium a perfect specimen of a pyroelectric

28 ...

26

**Crystals**whose natural primitive cells have a nonvanishing dipole moment poare called pyroelectric . 27 In equilibrium a perfect specimen of a pyroelectric

**crystal**has a total dipole moment of Po times the number of cells in the**crystal**,28 ...

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### Contents

The Drude Theory of Metals | 1 |

Free electron densities and ra | 5 |

Thermal conductivities | 21 |

Copyright | |

46 other sections not shown

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### Common terms and phrases

additional applied approximation assume atomic band boundary Bragg Bravais lattice calculation carrier Chapter charge close collisions compared completely condition conduction consider constant containing contribution correction crystal cubic density dependence derivation described determined direction discussion distribution effect electric field elements energy equal equation equilibrium example fact Fermi surface Figure follows free electron frequency given gives heat hexagonal holes important independent integral interaction ionic ions known lattice vector leading levels limit linear magnetic field mean measured metals method momentum motion normal Note observed occupied orbits perpendicular phonon plane positive possible potential present primitive cell problem properties reciprocal lattice reflection region relation requires result satisfy scattering semiclassical Show shown simple single solid solution space specific structure symmetry Table temperature term theory thermal vanishes volume wave functions wave vector zero zone