## Solid state physics |

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Page 8

1-6 Crystal Directions and Planes Directions in crystals are usually represented

in shorthand by three

\a\ + U2<iJ + »3<ik in a cubic crystal, for example, is written as [ni,n2,ns].

1-6 Crystal Directions and Planes Directions in crystals are usually represented

in shorthand by three

**integers**inside a set of square brackets. The direction R = ti\a\ + U2<iJ + »3<ik in a cubic crystal, for example, is written as [ni,n2,ns].

Page 11

the distance between the centers of nearest-neighbor atoms is the diameter of

the atoms. Thus, in this hypothetical crystal, the diameter of the atoms is 5.00 A.

Planes of atoms in a crystal are usually represented in shorthand by three

the distance between the centers of nearest-neighbor atoms is the diameter of

the atoms. Thus, in this hypothetical crystal, the diameter of the atoms is 5.00 A.

Planes of atoms in a crystal are usually represented in shorthand by three

**integers**...Page 72

Also, as before, we label the atoms with

in Fig. 3-12). However, here we label atoms of mass mi with even

+ 2, etc.) and atoms of mass m2 with odd

Also, as before, we label the atoms with

**integers**(2n - 1, 2n, 2n + 1, 2n + 2, 2n + 3in Fig. 3-12). However, here we label atoms of mass mi with even

**integers**(2n, 2n+ 2, etc.) and atoms of mass m2 with odd

**integers**(2n - 1, 2n + 1, 2n + 3, etc.).### 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