## Introduction to Solid State Physicsproblems after each chapter |

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Page 4

We choose coordinate axes so that a is parallel to the x axis . If now we rotate a by an angle 0 , we get a new

We choose coordinate axes so that a is parallel to the x axis . If now we rotate a by an angle 0 , we get a new

**vector**a ' with components az ' = a cos ; ay ' = a sin 0 . а If the lattice is invariant under the rotation 0 , the**vector**a ...Page 50

The

The

**vector**r * ( hkl ) in the reciprocal lattice is in the same direction but n times as long as the**vector**corresponding to the true crystal plane . That is , the nth point from the origin in a given row in the reciprocal lattice ...Page 545

The resulting strain pattern is that of the dislocation characterized jointly by the boundary curve and the Burgers

The resulting strain pattern is that of the dislocation characterized jointly by the boundary curve and the Burgers

**vector**. It is clear that the Burgers**vector**must be one of a discrete set of lattice**vectors**that will allow the ...### 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 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 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