## Introduction to Solid State Physics |

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Page 22

ATOMIC

depends on a number of factors. One of these is the atomic

which describes Incident monochromatic beam Fig. 1.15. Schematic diagram of a

rotating ...

ATOMIC

**SCATTERING**FACTOR The intensity of a given diffracted wavedepends on a number of factors. One of these is the atomic

**scattering**factor,which describes Incident monochromatic beam Fig. 1.15. Schematic diagram of a

rotating ...

Page 264

where B is the amplitude;10 we suppose that r is sufficiently far from To so that in

the vicinity of r the

direction k. The amplitude B will be proportional to the strength of the incident

wave at ...

where B is the amplitude;10 we suppose that r is sufficiently far from To so that in

the vicinity of r the

**scattered**wave may 'be treated as a plane wave in thedirection k. The amplitude B will be proportional to the strength of the incident

wave at ...

Page 282

MOBILITY IN THE PRESENCE OF IMPURITY ATOMS When relatively few

impurity atoms are present, or at high temperatures, lattice

determine the mobility. At higher impurity concentrations, electron

impurity atoms ...

MOBILITY IN THE PRESENCE OF IMPURITY ATOMS When relatively few

impurity atoms are present, or at high temperatures, lattice

**scattering**willdetermine the mobility. At higher impurity concentrations, electron

**scattering**byimpurity atoms ...

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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