## 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 18

The alkali metals have , in fact , been

ultraviolet . A numerical evaluation of ( 1 . 38 ) gives the frequency at which

transparency should set in as ( 1 . 40 ) I - 3 / 2 Vo = * = 11 . 4 ~ ( " x 1015 Hz Or 10

= F = 0 .

The alkali metals have , in fact , been

**observed**to become transparent in theultraviolet . A numerical evaluation of ( 1 . 38 ) gives the frequency at which

transparency should set in as ( 1 . 40 ) I - 3 / 2 Vo = * = 11 . 4 ~ ( " x 1015 Hz Or 10

= F = 0 .

Page 101

Diffraction peaks corresponding to reciprocal lattice vectors K will be

only if K gives a reciprocal lattice point on ... the Ewald construction confirms our

Diffraction peaks corresponding to reciprocal lattice vectors K will be

**observed**only if K gives a reciprocal lattice point on ... the Ewald construction confirms our

**observation**that for a general incident wave vector there will be no Bragg peaks .Page 383

Leaving aside , for the moment , these exceptions , this shows that the

lattice constants can be reproduced to a ... resolved and the anomalous behavior

of the lithium halides can be explained by the following further

Leaving aside , for the moment , these exceptions , this shows that the

**observed**lattice constants can be reproduced to a ... resolved and the anomalous behavior

of the lithium halides can be explained by the following further

**observation**: Our ...### What people are saying - Write a review

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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

### Other editions - View all

Solid State Physics: Advances in Research and Applications, Volume 42 Henry Ehrenreich Limited preview - 1989 |

### 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