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

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Page 36

Each atom has four

are eight atoms in a unit cube. The diamond lattice is relatively empty; the

maximum proportion of the available volume which may be filled by hard spheres

is ...

Each atom has four

**nearest neighbors**and twelve next-**nearest neighbors**. Thereare eight atoms in a unit cube. The diamond lattice is relatively empty; the

maximum proportion of the available volume which may be filled by hard spheres

is ...

Page 67

That is, each carbon atom will be at the center of the tetrahedron formed by the

typical examples of the tetrahedral covalent bond. The diamond structure is

loosely ...

That is, each carbon atom will be at the center of the tetrahedron formed by the

**nearest neighbor**atoms. Diamond (Figs. 1.27 and 1.28) and methane, CH4, aretypical examples of the tetrahedral covalent bond. The diamond structure is

loosely ...

Page 97

If a is the

homogeneous pure strain V = ^ (ezz* + evv* + ej) + ^ (eyt* + ej + O, where N is

the atomic concentration. On comparison with (4.22) we see that our model leads

to ...

If a is the

**nearest neighbor**distance, we may write for the energy density for ahomogeneous pure strain V = ^ (ezz* + evv* + ej) + ^ (eyt* + ej + O, where N is

the atomic concentration. On comparison with (4.22) we see that our model leads

to ...

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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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### Common terms and phrases

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