## 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 153

3 ) requires for each K that either Ck - K = 0 or E = ER - K . The latter possibility

can occur for only a single K , unless it happens that some of the & - K are

for several different choices of K . If such degeneracy does not occur , then we ...

3 ) requires for each K that either Ck - K = 0 or E = ER - K . The latter possibility

can occur for only a single K , unless it happens that some of the & - K are

**equal**for several different choices of K . If such degeneracy does not occur , then we ...

Page 276

For example , electrons on orbits with diameters

Figure 14 . 7a ) can be accelerated ( or decelerated ) by the wave throughout

their entire orbit , while electrons with orbit diameters

wavelength ...

For example , electrons on orbits with diameters

**equal**to half a wavelength (Figure 14 . 7a ) can be accelerated ( or decelerated ) by the wave throughout

their entire orbit , while electrons with orbit diameters

**equal**to a wholewavelength ...

Page 620

( b ) An ionic crystal with point defects of the Schottky type (

positive and negative ion vacancies ) . ( c ) An ionic crystal with defects of the

Frenkel type (

1 1 + 1 ...

( b ) An ionic crystal with point defects of the Schottky type (

**equal**numbers ofpositive and negative ion vacancies ) . ( c ) An ionic crystal with defects of the

Frenkel type (

**equal**numbers of positive ion vacancies and interstitials ) 1 + + 1 +1 1 + 1 ...

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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