## 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 12

This state of stress should appear as a transverse voltage (

Hall voltage ) , which Hall was able to observe . Hall ' s experiment is depicted in

Figure 1 . 3 . An electric field Ex is applied to a wire extending in the x - direction ...

This state of stress should appear as a transverse voltage (

**known**today as theHall voltage ) , which Hall was able to observe . Hall ' s experiment is depicted in

Figure 1 . 3 . An electric field Ex is applied to a wire extending in the x - direction ...

Page 142

If the band gap is comparable to koT , the solid is

semiconductor ( Chapter 28 ) . Because the number of levels in a mitive some

levels band is equal to the number of primitive cells in the crystal ( page 136 )

and because ...

If the band gap is comparable to koT , the solid is

**known**as an intrinsicsemiconductor ( Chapter 28 ) . Because the number of levels in a mitive some

levels band is equal to the number of primitive cells in the crystal ( page 136 )

and because ...

Page 331

7 ) ( there is one for each occupied one - electron level 4 ; ( r ) ) is

Hartree equations . These nonlinear equations for the one - electron wave

functions and energies are solved , in practice , by iteration : A form is guessed

for Uel ...

7 ) ( there is one for each occupied one - electron level 4 ; ( r ) ) is

**known**as theHartree equations . These nonlinear equations for the one - electron wave

functions and energies are solved , in practice , by iteration : A form is guessed

for Uel ...

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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