## Solid state physics |

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Page 99

By this, we mean that the energy can only take on certain discrete

postulated that these allowed

frequency of the wave, h is a proportionality constant called Planck's constant,

and n is any ...

By this, we mean that the energy can only take on certain discrete

**values**. Hepostulated that these allowed

**values**of energy are E - nhu, where u is thefrequency of the wave, h is a proportionality constant called Planck's constant,

and n is any ...

Page 134

If we require xJj to satisfy the boundary conditions of Eq. (7-1), we find that the

components of k must be restricted to

n2(n/L), where nx, ny, n2 are integers. As in the one-dimensional case, we ...

If we require xJj to satisfy the boundary conditions of Eq. (7-1), we find that the

components of k must be restricted to

**values**, kx = nx(n/L), ky = nv{x/L), (7-4) kz =n2(n/L), where nx, ny, n2 are integers. As in the one-dimensional case, we ...

Page 287

(See Appendix 7 for

proportional to the critical temperature: Superconductors with large gap energies

maintain superconductivity to higher temperatures. Problem 13-6. Using Eq. 13-

11 ...

(See Appendix 7 for

**values**of 2 A.) BCS theory predicts that the gap energy isproportional to the critical temperature: Superconductors with large gap energies

maintain superconductivity to higher temperatures. Problem 13-6. Using Eq. 13-

11 ...

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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