## Introduction to Solid State Physicsproblems after each chapter |

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Page 273

forms , of equal parts of

forms , of equal parts of

**waves**traveling to the right ( eiti / a ) and to the left ( e - ir / a ) . ... 42 correspond to different values of the energy , even though the functions have the same values of the**wave**vector . In Fig .Page 274

**wave**. If the potential energies of y 1 and 2 differ by an amount AE we have , referring to Fig . 11.1 ( b ) , an energy gap of width AE . The**wave**function at points A will be 42 , and the**wave**function above the energy gap at points B ...Page 284

**WAVE**FUNCTIONS FOR ZERO**WAVE**VECTOR It may appear to the reader that there is a certain inconsistency between the discussion of the preceding chapter , in which we emphasized the usefulness of the free electron model as applied to 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