## Introduction to Solid State Physics |

### From inside the book

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Page 17

There are 230

theory of space groups in order to understand the crystal structures explicitly

discussed ...

There are 230

**possible**space groups . A full discussion of space groups is not**possible**in the space available here . We shall not require knowledge of thetheory of space groups in order to understand the crystal structures explicitly

discussed ...

Page 33

It is not

is it

terms in the series that the contributions from the positive and negative terms

nearly ...

It is not

**possible**to write down the successive terms by a casual inspection , noris it

**possible**to sum the series conveniently . It is important so to arrange theterms in the series that the contributions from the positive and negative terms

nearly ...

Page 104

It is not

X - rays , because of the low scattering power of hydrogen . Neutron diffraction is

a

It is not

**possible**to determine the position of hydrogen atoms in a crystal by usingX - rays , because of the low scattering power of hydrogen . Neutron diffraction is

a

**possible**tool , especially if deuterium is substituted for hydrogen .### What people are saying - Write a review

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### Contents

LATTICE ENERGY OF IONIC CRYSTALS | 29 |

ELASTIC CONSTANTS OF CRYSTALS | 43 |

LATTICE VIBRATIONS | 60 |

Copyright | |

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### Common terms and phrases

alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero