## Solid state physics |

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Page 7

choice of position of the

arrange the cubes so that each cube contains one

Fig. 1-7a). Alternately, we may arrange the cubes so that the

the ...

choice of position of the

**lattice point**within the unit cell, is arbitrary. We mayarrange the cubes so that each cube contains one

**lattice point**at its center (seeFig. 1-7a). Alternately, we may arrange the cubes so that the

**lattice points**are atthe ...

Page 12

Note that every

original sc

Note that every

**lattice point**is equivalent to every other**lattice point**. Each of theoriginal sc

**lattice points**is also in the body-centered position of eight of the new**lattice points**. The conventional unit cell for the bcc lattice is a cube of side a as ...Page 22

1-20, we can see that the Na sites form a set of

. We cannot tell the difference between Na atoms. They are each in identical

surroundings. Such a set of

1-20, we can see that the Na sites form a set of

**lattice points**which are equivalent. We cannot tell the difference between Na atoms. They are each in identical

surroundings. Such a set of

**lattice points**which are equivalent to each other is ...### What people are saying - Write a review

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### Contents

XRay Diffraction | 37 |

Lattice Vibrations | 61 |

Classical Model of Metals | 89 |

Copyright | |

12 other sections not shown

### Common terms and phrases

Answer Appendix basis vectors bcc lattice bond Bragg angle Bragg's Law Bravais lattice Brillouin zone called Chapter collisions conduction electrons Consider conventional unit cell Cooper pairs depletion layer diode direction dispersion curve displacement distance doped effective mass elec electric current electric field electrons and holes emitter energy band equal example Fermi energy Fermi level Fermi surface force forward biased free electron free particle frequency given by Eq inside integers ions k-space laser lattice parameter lattice points lattice vector lattice wave magnetic field n-type semiconductor NaCl negative neutrons number of electrons obtain occupied one-dimensional oscillate p-n junction photon positively charged potential energy primitive unit cell Problem rays reciprocal lattice reverse biased sc lattice scattered Schroedinger's equation shown in Fig sodium metal solid structure superconductor temperature tion transistor trons unit cell unoccupied values velocity voltage wave function wave number wave vector wavelength Wigner-Seitz cell wire x-ray diffraction zero