## Introduction to Solid State Physics |

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Page 79

jxe-v/kTdx s $e-"1,kT[x + (gx*/kT) + (fx6/kT)]dx = (g/kT)(kT/c)*(3T»/4); $e-v/kTdx9

*$e-exVkT dx = (xlbT/c)**; so that (5.24) I = ZkTg/4c2, giving a constant value of

the temperature coefficient of

...

jxe-v/kTdx s $e-"1,kT[x + (gx*/kT) + (fx6/kT)]dx = (g/kT)(kT/c)*(3T»/4); $e-v/kTdx9

*$e-exVkT dx = (xlbT/c)**; so that (5.24) I = ZkTg/4c2, giving a constant value of

the temperature coefficient of

**thermal**expansion. Values of the linear expansion...

Page 81

Values of the Gruneisen 7

useful in discussing the conduction of

introduce (following Debye) the concept of the mean free path of the lattice waves

or ...

Values of the Gruneisen 7

**THERMAL**CONDUCTIVITY IN NON-METALS It isuseful in discussing the conduction of

**thermal**energy in dielectric substances tointroduce (following Debye) the concept of the mean free path of the lattice waves

or ...

Page 84

an important mechanism in determining the mean free path, anhar- monic

interaction is the only mechanism in solids whereby the frequency distribution of

phonons may be brought into

needs ...

an important mechanism in determining the mean free path, anhar- monic

interaction is the only mechanism in solids whereby the frequency distribution of

phonons may be brought into

**thermal**equilibrium. In**thermal**conductivity oneneeds ...

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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

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