## Introduction to Solid State Physicsproblems after each chapter |

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Page 18

plane normal to the principal axis , the outer circle is heavy on the symmetry

element stereogram . Symmetry axes perpendicular to the principal axis are

denoted by ...

**Reflection**planes are indicated by heavy lines . If there is present a**reflection**plane normal to the principal axis , the outer circle is heavy on the symmetry

element stereogram . Symmetry axes perpendicular to the principal axis are

denoted by ...

Page 48

We recall that a , b , y are the direction cosines of S , the normal to the

plane , referred to the basis vectors a , b ... maxima occur when the scattering

direction may be derived from the incident direction by

.

We recall that a , b , y are the direction cosines of S , the normal to the

**reflecting**plane , referred to the basis vectors a , b ... maxima occur when the scattering

direction may be derived from the incident direction by

**reflection**in a lattice plane.

Page 271

We have seen in the earlier discussions of x - ray and elastic wave propagation

in crystals that Bragg

propagation in periodic structures . Bragg

We have seen in the earlier discussions of x - ray and elastic wave propagation

in crystals that Bragg

**reflection**is an important and characteristic feature of wavepropagation in periodic structures . Bragg

**reflection**occurs also for 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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alloys applied approximately associated atoms axes axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone