## 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 352

74 ) into the Fourier

) and evaluating that

best done as a contour

...

74 ) into the Fourier

**integral**dk VAP = Seni et " V ( B ) V ( r ) = eik . V ( k ) ( 17 . 75) and evaluating that

**integral**in spherical coordinates . ( The radial**integral**isbest done as a contour

**integral**. ) ( c ) Deduce from ( 17 . 74 ) that Vo ( r ) satisfies...

Page 530

We may exploit this fact to simplify the correction term by writing the

k ' as an

surfaces & = E . As & varies , the variation of the term in 1 & - Er in the

denominator of ...

We may exploit this fact to simplify the correction term by writing the

**integral**overk ' as an

**integral**over energy E and an**integral**over the constant - energysurfaces & = E . As & varies , the variation of the term in 1 & - Er in the

denominator of ...

Page 762

has the periodicity of the lattice ( K being a reciprocal lattice vector ) its

over a primitive cell is independent of the choice of cell . ? In particular , it will not

be changed if we translate the primitive cell C through a vector d ( not necessarily

...

has the periodicity of the lattice ( K being a reciprocal lattice vector ) its

**integral**over a primitive cell is independent of the choice of cell . ? In particular , it will not

be changed if we translate the primitive cell C through a vector d ( not necessarily

...

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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