## 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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Results 1-3 of 78

Page 222

This is a direct consequence of the semiclassical analogue of Liouville ' s

theorem , which asserts the following : 17 Given any

phase space 12 , , consider the point r ' , k ' into which each point r , k in S2 , is

taken by ...

This is a direct consequence of the semiclassical analogue of Liouville ' s

theorem , which asserts the following : 17 Given any

**region**of six - dimensionalphase space 12 , , consider the point r ' , k ' into which each point r , k in S2 , is

taken by ...

Page 540

3 In calculating the local field at a point r it is convenient to consider separately

contributions from the far

radius r , about r and all external sources of field ) and from the near

, all ...

3 In calculating the local field at a point r it is convenient to consider separately

contributions from the far

**region**( i . e . , all the crystal outside the sphere ofradius r , about r and all external sources of field ) and from the near

**region**( i . e ., all ...

Page 591

The term “ junction ” is used to refer both to the device as a whole and , more

specifically , to the transition

nonuniform . As we shall see below , the nonuniformity in impurity concentrations

...

The term “ junction ” is used to refer both to the device as a whole and , more

specifically , to the transition

**region**about x = 0 in which the doping profile isnonuniform . As we shall see below , the nonuniformity in impurity concentrations

...

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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