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

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Page 44

interact with atoms and which have a wavelength comparable with the

interatomic spacing in crystals; that is, we require a wavelength of the order of 1 A

(= 10~8 ...

**X**-**Rays**. by. Crystals. To explore the structure of crystals we require waves whichinteract with atoms and which have a wavelength comparable with the

interatomic spacing in crystals; that is, we require a wavelength of the order of 1 A

(= 10~8 ...

Page 49

INTERFERENCE CONDITIONS AND THE RECIPROCAL LATTICE* The

conditions for an

elegant form with the help of the reciprocal lattice transformation. The reciprocal

lattice is ...

INTERFERENCE CONDITIONS AND THE RECIPROCAL LATTICE* The

conditions for an

**x**-**ray**beam to be diffracted by a crystal may be expressed in anelegant form with the help of the reciprocal lattice transformation. The reciprocal

lattice is ...

Page 55

EXPERIMENTAL

, for

wavelength X striking a crystal at an arbitrary angle of incidence in general will

not be ...

EXPERIMENTAL

**X**-**RAY**DIFFRACTION METHODS The Bragg law, 2d sin 8 = nX, for

**x**-**ray**diffraction requires that 8 and X be matched; that is,**x**-**rays**ofwavelength X striking a crystal at an arbitrary angle of incidence in general will

not be ...

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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