By Edward D. Palik
Whereas bits and items of the index of refraction n and extinction coefficient okay for a given fabric are available in numerous handbooks, the guide of Optical Constants of Solids supplies for the 1st time a unmarried set of n and okay values over the broadest spectral variety (ideally from x-ray to mm-wave region). The critiquers have selected the numbers for you, in response to their very own wide event within the learn of optical houses. even if you would like one quantity at one wavelength or many numbers at many wavelengths, what's to be had within the literature is condensed down right into a unmarried set of numbers. * individuals have made up our minds the easiest values for n and okay* References in each one critique let the reader to return to the unique information to envision and comprehend the place the values have come from* permits the reader to figure out if any info in a spectral quarter has to be crammed in* offers a large and designated view of experimental ideas for measuring the optical constants n and ok* accommodates and describes crystal constitution, space-group symmetry, unit-cell dimensions, variety of optic and acoustic modes, frequencies of optic modes, the irreducible illustration, band hole, plasma frequency, and static dielectric consistent
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Extra info for Handbook of Optical Constants of Solids, Five-Volume Set: Handbook of Optical Constants of Solids: Volume 1 (Academic Press Handbook)
Example text
5 (neglecting retardation and relativistic effects) [51]. (For more information see Bethe et al. [24] and Rau et al. ) In discussing the optical properties of metals and superconductors, it is common to rewrite the rules in terms of the complex frequency-dependent conductivity as tr(og) = -(iog/4rc)e(co). (17) The f sum rule then takes the form fo~ tr(~o) do9 7z ~ e 2 2 m (18) This rule and its generalizations [-9, 52] as well as related rules for the surface impedance [53, 54-] have been used extensively to relate the difference in conductivity between the superconducting and the normal states in the region of the superconducting gap to the 6-function conductivity at zero frequency in superconductors [53, 55-57].
They are, therefore, currently of little practical value since the phase is generally not measured. The phase and amplitude may be separated by considering the analytic function In ~(fO) = In r(fO) + iO(fO). (57) There is, however, a major difference between this and the dielectric function, refractive index, and so on. The latter approach unity as co ~ oo, whereas In f(fo) diverges logarithmically since lim,,_,oo r(fO)= 0. Thus, the dispersion relations and sum rules for In f(o) are not of the same form as those for e(o~) or U(fO).
24, 417 (1971). Chapter 3 Dispersion Theory, Sum Rules, and Their Application to the Analysis of Optical Data* D. Y. Smith Argonne National Laboratory Argonne, Illinois and M a x - P l a n c k - l n s t i t u t for F e s t k ~ r p e r f o r s c h u n g Stuttgart, Federal Republic of Germany I. Introduction II. Optical Sum Rules and Their Physical Interpretation A. Superconvergence Sum Rules for ~(~) B. Superconvergence Sum Rules for N(~o) C. Superconvergence Sum Rules for Functions of N and D. Superconvergence Relations Employing Weighting Functions E.