## Introduction to solid state physics |

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Page 23

If each of the points lies on a crystal

the positions of the points along the

example, the atoms determining the plane have coordinates (4, 0, 0), (0, 1, 0), (0,

0, ...

If each of the points lies on a crystal

**axis**, the plane may be specified by givingthe positions of the points along the

**axes**in terms of the lattice constants. If, forexample, the atoms determining the plane have coordinates (4, 0, 0), (0, 1, 0), (0,

0, ...

Page 32

Threefold

stacking of tetrahedral layers in cubic and hexagonal ZnS. The large atoms are S;

the small atoms are Zn. The vertical

Threefold

**axis**s- i nreeioia i r [in] - Sixfold**axis**c Cubic Hexagonal Figure 31 Thestacking of tetrahedral layers in cubic and hexagonal ZnS. The large atoms are S;

the small atoms are Zn. The vertical

**axis**of hexagonal ZnS is a six-fold screw ...Page 164

1.0 0.8 0.6 i 0.4 | 0.2 o 1.0 N X « o 0.8 0.6 § 0.4 | | 0.2 0 0.2 0.4 0.6 0.8 1.0 K/KmM,

in [110] direction Figure 5 Dispersion curves determined by the inelastic

scattering of x-rays for phonons propagating along the [ 1 10]

1.0 0.8 0.6 i 0.4 | 0.2 o 1.0 N X « o 0.8 0.6 § 0.4 | | 0.2 0 0.2 0.4 0.6 0.8 1.0 K/KmM,

in [110] direction Figure 5 Dispersion curves determined by the inelastic

scattering of x-rays for phonons propagating along the [ 1 10]

**axis**in aluminum.### What people are saying - Write a review

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### Contents

CRYSTAL STRUCTURE | 1 |

CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |

CRYSTAL BINDING | 95 |

Copyright | |

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absolute zero absorption alkali alloy antiferromagnet applied field applied magnetic field atoms axis boundary Brillouin zone calculated Chapter charge components conduction band conduction electrons critical field crystal structure cubic defined density dielectric constant diffraction dipole direction dislocation dispersion relation elastic electric field electron gas energy gap entropy equation equilibrium excited exciton experimental F center Fermi surface ferroelectric ferromagnetic Figure free electron frequency function given heat capacity hole impurity interaction ionic ions lattice constant lattice points low temperatures magnetic field magnon Meissner effect metal momentum motion nearest neighbors neutron normal nuclear nucleus optical orbital paramagnetic particle phase phonon Phys physics plane polarizability polarization positive potential primitive cell quantum reciprocal lattice vector region resonance result room temperature scattering semiconductor shown in Fig solid specimen sphere spin superconducting susceptibility theory thermal tion transition temperature unit vacancies valence band velocity wave wavefunction wavelength wavevector x-ray