## Introduction to Solid State Physics |

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Page 13

A convenient way of choosing the

draw the various vectors ni& + n2b + n3c and then bisect each vector with a

plane perpendicular to it. The region of space which can be reached from 0

without ...

A convenient way of choosing the

**unit cell**is to choose an origin 0 and from itdraw the various vectors ni& + n2b + n3c and then bisect each vector with a

plane perpendicular to it. The region of space which can be reached from 0

without ...

Page 14

The positions of points in a

which each coordinate is a fraction of the axial length, a, b, or c, in the direction of

the coordinate, with the origin taken at the corner of a

The positions of points in a

**unit cell**are specified in terms of lattice coordinates, inwhich each coordinate is a fraction of the axial length, a, b, or c, in the direction of

the coordinate, with the origin taken at the corner of a

**unit cell**. Thus the ...Page 16

The

atom added within the prism, so that the hcp

DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;

i i i ...

The

**unit cell**of the hcp structure is the hexagonal primitive cell but with an extraatom added within the prism, so that the hcp

**unit cell**contains two atoms.DIAMOND STRUCTURE The space lattice of diamond is fcc with two atoms 000 ;

i i i ...

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### Contents

LATTICE ENERGY OF IONIC CRYSTALS | 29 |

ELASTIC CONSTANTS OF CRYSTALS | 43 |

LATTICE VIBRATIONS | 60 |

Copyright | |

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alkali alloy antiferromagnetic applied approximation atoms axes axis barium titanate boundary Brillouin zones calculated charge coefficient conduction band consider crystal structure cube cubic crystal Curie point curve Debye density diamagnetic dielectric constant diffraction dipole direction discussed dislocation displacement distribution domain effect elastic electric field entropy equation equilibrium experimental F-centers factor Fermi ferroelectric ferromagnetic free electron frequency heat capacity holes impurity interaction ionic crystals ions lattice constant lattice points London low temperatures magnetic field mean free path metals molecules motion nearest neighbor normal observed orbital parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potential Proc quantum ratio region resonance result room temperature rotation scattering Seitz shear Shockley shown in Fig simple cubic single crystal sodium chloride solids specimen spin superconducting susceptibility symmetry theory thermal tion unit cell unit volume valence values vector velocity wave functions wavelength x-ray zero