## Introduction to Solid State Physicsproblems after each chapter |

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Page 268

TABLE 10.8 . Work FUNCTIONS FROM PHOTOELECTRIC DATA Metal • ( ev )

Na 2.3 K 2.26 Cr 4.37 Zn 4.24 4. 19 Pt 6.2 PROBLEMS 10.1 . ( a ) Using the

boundary condition y = 0 on the surfaces of a cube of side L , find all the

functions ...

TABLE 10.8 . Work FUNCTIONS FROM PHOTOELECTRIC DATA Metal • ( ev )

Na 2.3 K 2.26 Cr 4.37 Zn 4.24 4. 19 Pt 6.2 PROBLEMS 10.1 . ( a ) Using the

boundary condition y = 0 on the surfaces of a cube of side L , find all the

**wave**functions ...

Page 274

referring to Fig . 11.1 ( b ) , an energy gap of width AE . The

points A will be 42 , and the

be 41 .

**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 atpoints A will be 42 , and the

**wave**function above the energy gap at points B willbe 41 .

Page 302

here follows the elementary approximate presentation by Weisskopf ; 15 the low

temperature theory is discussed in Appendix K. If the lattice of a metal is perfect

and there are no lattice vibrations , the electron

here follows the elementary approximate presentation by Weisskopf ; 15 the low

temperature theory is discussed in Appendix K. If the lattice of a metal is perfect

and there are no lattice vibrations , the electron

**waves**pass through the lattice ...### 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