## Solid State PhysicsThis book provides an introduction to the field of solid state physics for undergraduate students in physics, chemistry, engineering, and materials science. |

### From inside the book

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Page 320

13 ) dt or coll This is the celebrated Boltzmann equation . The

side are often referred to as the drift

collision

Boltzmann ...

13 ) dt or coll This is the celebrated Boltzmann equation . The

**terms**on the leftside are often referred to as the drift

**terms**, and the**term**on the right side as thecollision

**term**. When the form ( 16 . 8 ) is used for the collision**term**, theBoltzmann ...

Page 648

20 ) to particular cases , we first observe that unless the

vanishes identically ( as it sometimes does ) , it will almost always be the

dominant

vanish , ( n ...

20 ) to particular cases , we first observe that unless the

**term**that is linear in Hvanishes identically ( as it sometimes does ) , it will almost always be the

dominant

**term**even when the field is very strong ( ~ 104 gauss ) . If it does notvanish , ( n ...

Page 766

3 ) , we can express ( E . 8 ) in

. ... 2 The first

3 ) , we can express ( E . 8 ) in

**terms**of Bloch functions : gal , baxt 5 LG * C * 2 ) el. ... 2 The first

**term**on the right of ( E . 8 ) comes from placing the second - order**term**in Hk + q ( Eq . ( E . 2 ) ) into the first - order**term**in the perturbation theory ...### 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