## Introduction to Solid State Physicsproblems after each chapter |

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Page 74

The definition of the Madelung constant a is , from Eq . ( 3.3 ) , Σ ( ( + ) Pij ] where

now , if we take the

used for positive ions and the minus sign for negative ions . An equivalent

definition ...

The definition of the Madelung constant a is , from Eq . ( 3.3 ) , Σ ( ( + ) Pij ] where

now , if we take the

**reference**ion as a negative charge , the plus sign will beused for positive ions and the minus sign for negative ions . An equivalent

definition ...

Page 117

Clarendon Press , Oxford , 1954 . L. Brillouin , Wave propagation in periodic

structures , McGraw - Hill Book Co. , New York , 1946 . C. Schaefer and F.

Matossi , Das ...

**REFERENCES**M. Born and K. Huang , Dynamical theory of crystal lattices ,Clarendon Press , Oxford , 1954 . L. Brillouin , Wave propagation in periodic

structures , McGraw - Hill Book Co. , New York , 1946 . C. Schaefer and F.

Matossi , Das ...

Page 573

G2 / 4 " The potential to at the

distribution is ( A.10 ) to = $ o * ( tar ” dr ) ( p / r ) = 29 : ( n / a ) " } , and so 4T ( A.11

) Hi ( i ) S ( GG - ? - Go / 47 AS 29 : ) . The potential ¥ 2 is to be evaluated at the ...

G2 / 4 " The potential to at the

**reference**ion point i due to the central Gaussiandistribution is ( A.10 ) to = $ o * ( tar ” dr ) ( p / r ) = 29 : ( n / a ) " } , and so 4T ( A.11

) Hi ( i ) S ( GG - ? - Go / 47 AS 29 : ) . The potential ¥ 2 is to be evaluated at the ...

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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