## Introduction to Solid State Physicsproblems after each chapter. |

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Results 1-3 of 31

Page 306

Roy. Soc. (London) A202, 103 (1950)]. *

(11.1) and the Kronig-Penney problem, that the energy discontinuities in the

monatomic one-dimensional lattice occur when the wave number satisfies (11.93

) k ...

Roy. Soc. (London) A202, 103 (1950)]. *

**BRILLOUIN ZONES**We have seen, from(11.1) and the Kronig-Penney problem, that the energy discontinuities in the

monatomic one-dimensional lattice occur when the wave number satisfies (11.93

) k ...

Page 316

We are therefore led to consider the second

First and second

is no discontinuity in energy across the top and bottom faces of the first zone if ...

We are therefore led to consider the second

**Brillouin zone**. The second Fig. 12.1.First and second

**Brillouin zones**for the hexagonal close-packed structure. Thereis no discontinuity in energy across the top and bottom faces of the first zone if ...

Page 326

Jones pointed out that the observed limit of the a phase (fee) occurs very close to

the electron concentration of 1.36 for which the inscribed Fermi sphere makes

contact with the

Jones pointed out that the observed limit of the a phase (fee) occurs very close to

the electron concentration of 1.36 for which the inscribed Fermi sphere makes

contact with the

**Brillouin zone**surface for the fee lattice. The observed electron ...### What people are saying - Write a review

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

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absorption acceptors alkali alloy approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point levels low temperatures magnetic field metals molecules motion nearest neighbor normal observed orbital p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc recombination region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero