## Introduction to Solid State Physicsproblems after each chapter |

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Page 6

( a ) Square

Rectangular

shown for both the primitive cell and for the rectangular unit cell , for which lal +

lbl ...

( a ) Square

**lattice**lal = bl ; y = 90° ( 6 ) Hexagonal**lattice**lal = Tbl ; y = 120° ( c )Rectangular

**lattice**lal # Ibl ; y = 90° ( d ) Centered rectangular**lattice**; axes areshown for both the primitive cell and for the rectangular unit cell , for which lal +

lbl ...

Page 26

In the triclinic system the single space

three axes of unequal lengths and unequal angles . The symmetry of the

ī , all space

In the triclinic system the single space

**lattice**has a primitive ( P ) unit cell , withthree axes of unequal lengths and unequal angles . The symmetry of the

**lattice**isī , all space

**lattices**being invariant under inversion . In the monoclinic system ...Page 51

As an example we show that a foc

direct fcc

is a / 2 , where a is the

As an example we show that a foc

**lattice**has as its reciprocal a bcc**lattice**. In thedirect fcc

**lattice**the distance between**lattice**planes in each cube edge directionis a / 2 , where a is the

**lattice**constant ; thus there are points in the reciprocal ...### 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 |

Copyright | |

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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 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