## Introduction to Solid State Physics |

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Page 374

If we had taken circularly polarized radiation in place on plane-polarized

radiation, the

selective absorption of one of the two circular components of a plane wave; the

other ...

If we had taken circularly polarized radiation in place on plane-polarized

radiation, the

**ratio**would have been unity. The factor one-half represents theselective absorption of one of the two circular components of a plane wave; the

other ...

Page 409

electron spin the magnetic moment is up = eh/2mc, and the angular momentum is

h/2; ...

**ratio**of the magnetic moment to the angular momentum. It is useful to equate the**ratio**to g'e/2mc, where g' is called the magnetomechanical factor." For anelectron spin the magnetic moment is up = eh/2mc, and the angular momentum is

h/2; ...

Page 558

The value of AE passes through a maximum when d AE/dr = 0, or when (19.13)

2r b = G/a, showing that the

magnitude of the Burgers vector equals the

shear stress.

The value of AE passes through a maximum when d AE/dr = 0, or when (19.13)

2r b = G/a, showing that the

**ratio**of the diameter of the critical loop to themagnitude of the Burgers vector equals the

**ratio**of the shear modulus to theshear stress.

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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