## Introduction to Solid State Physics |

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Page 223

12

considerably from one metal to another, from sodium, which we may think of as a

sea of negative charge in which are embedded the positive ion cores, to tin and ...

12

**Free Electron**Theory of Metals The electronic structures of metals may differconsiderably from one metal to another, from sodium, which we may think of as a

sea of negative charge in which are embedded the positive ion cores, to tin and ...

Page 235

perature as the strongest field yet obtained, 5 X 105 oersteds, only corresponds

to a temperature of ~50°K. We now calculate the expression for the paramagnetic

susceptibility of a

perature as the strongest field yet obtained, 5 X 105 oersteds, only corresponds

to a temperature of ~50°K. We now calculate the expression for the paramagnetic

susceptibility of a

**free electron**gas. Following the notation of (12.23) and the ...Page 249

13 Band Theory of Metals The

preceding chapter gives us a good deal of insight into certain of the physical

properties of metals, yet there are other properties for which the

theory is ...

13 Band Theory of Metals The

**free electron**theory of metals developed in thepreceding chapter gives us a good deal of insight into certain of the physical

properties of metals, yet there are other properties for which the

**free electron**theory is ...

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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