## Solid state physics |

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Page 22

Such a set of lattice points which are equivalent to each other is called a

we can see in Fig. 1-20. Actually, the absolute location of the lattice points is ...

Such a set of lattice points which are equivalent to each other is called a

**Bravais****lattice**. The**Bravais lattice**of NaCl corresponds to the set of Na sites and is fcc aswe can see in Fig. 1-20. Actually, the absolute location of the lattice points is ...

Page 30

1-13 Other

structures exist which have

discussed.

1-13 Other

**Bravais Lattices**Since we were not successful in forming a new**Bravais lattice**with the diamond structure, we might wonder what other kinds ofstructures exist which have

**Bravais lattices**different from those we alreadydiscussed.

Page 50

Generally, then, Bragg's Law must be applied to points of the

crystal rather than to positions of atoms. The distance d in Eq. (2-10) refers to the

distance between planes of

Generally, then, Bragg's Law must be applied to points of the

**Bravais lattice**of acrystal rather than to positions of atoms. The distance d in Eq. (2-10) refers to the

distance between planes of

**Bravais lattice**points, rather than to planes of atoms.### What people are saying - Write a review

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### Contents

XRay Diffraction | 37 |

Lattice Vibrations | 61 |

Classical Model of Metals | 89 |

Copyright | |

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### 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