Introduction to Solid State Physicsproblems after each chapter |
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Page 44
Radiation of longer wavelength generally cannot resolve the details of structure
on an atomic scale , and radiation of much shorter wavelength is diffracted
through only very small angles , as seen from Eq . ( 2.1 ) below , although crystal
...
Radiation of longer wavelength generally cannot resolve the details of structure
on an atomic scale , and radiation of much shorter wavelength is diffracted
through only very small angles , as seen from Eq . ( 2.1 ) below , although crystal
...
Page 113
The wavelength at maximum reflection is known as the residual ray or Reststrahl
wavelength , and the selective reflection has been employed experimentally to
obtain narrow bands of radiation in the far infrared . Positions of the absorption ...
The wavelength at maximum reflection is known as the residual ray or Reststrahl
wavelength , and the selective reflection has been employed experimentally to
obtain narrow bands of radiation in the far infrared . Positions of the absorption ...
Page 125
For long wavelengths relative to the lattice spacing the ... The long wavelength
motions are particularly important at low temperatures , as there will always be
modes of vibration in an infinite crystal for which hw « kT , even though we may
have ...
For long wavelengths relative to the lattice spacing the ... The long wavelength
motions are particularly important at low temperatures , as there will always be
modes of vibration in an infinite crystal for which hw « kT , even though we may
have ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone