## 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 71

PRIMITIVE UNIT CELL A volume of space that , when translated through all the

vectors in a Bravais lattice , just fills all of space without either overlapping itself

or leaving voids is called a

is ...

PRIMITIVE UNIT CELL A volume of space that , when translated through all the

vectors in a Bravais lattice , just fills all of space without either overlapping itself

or leaving voids is called a

**primitive cell**or primitive unit cell of the lattice . Thereis ...

Page 72

this result holds for any

independent of the choice of cell . It also follows from the definition of a

first up into ...

this result holds for any

**primitive cell**, the volume of a**primitive cell**isindependent of the choice of cell . It also follows from the definition of a

**primitive****cell**that , given any two**primitive cells**of arbitrary shape , it is possible to cut thefirst up into ...

Page 73

UNIT CELL ; CONVENTIONAL UNIT CELL One can fill space up with

nonprimitive unit cells ( known simply as unit cells or ... The conventional unit cell

is generally chosen to be bigger than the

symmetry .

UNIT CELL ; CONVENTIONAL UNIT CELL One can fill space up with

nonprimitive unit cells ( known simply as unit cells or ... The conventional unit cell

is generally chosen to be bigger than the

**primitive cell**and to have the requiredsymmetry .

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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