## Introduction to Solid State Physics |

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Page 286

To satisfy these two

boundary planes of each polyhedron. ... The cubes show the unit cells in either

case. sphere is determined by the

To satisfy these two

**conditions**the normal derivative Óuo/ön must vanish on theboundary planes of each polyhedron. ... The cubes show the unit cells in either

case. sphere is determined by the

**condition**that the volume of the s sphere be ...Page 373

... we sa, for various relaxation times in units wr. Curves are given for both linear

polarization and circular polarization of the r-f field. It is interesting to state in

terms of the mobility the

resonance.

... we sa, for various relaxation times in units wr. Curves are given for both linear

polarization and circular polarization of the r-f field. It is interesting to state in

terms of the mobility the

**condition**at > 1 for the observation of cyclotronresonance.

Page 585

We note that the Bragg

also marks the boundaries on the KronigPenney model. At the boundary the

wave functions are standing waves which do not carry current. For k just above

the ...

We note that the Bragg

**condition**for reflection is also k = rm/a, and this**condition**also marks the boundaries on the KronigPenney model. At the boundary the

wave functions are standing waves which do not carry current. For k just above

the ...

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absorption acceptors alkali alloys approximately atoms axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transition unit volume vacancies valence band values vector velocity wave functions wavelength zero