By Edward D. Palik
"This e-book will function an invaluable reference. The editor and individuals deserve a degree of thank you for his or her attempt to facilitate for us the discovering values of the optical constants of 37 solids and for offering an in-one-placesummary of numerous suggestions for decision of n and ok. - R.M.A. Azzam and Jacqueline Casset in utilized OPTICS"The great thing about this publication is within the breadth of the spectral variety covered....The price of this compilation of significantly reviewed optical facts a long way outweighs the books deficiencies and...this guide has to be considered as a need in any physics or fabrics technological know-how reference library. - David M. Roessler, common automobiles learn Laboratories, Warren, Michigan, in OPTICAL NEWS"The editor ready a desk that summarizes the optical houses of the fabrics reviewed in Volumes. I and II. the volume of the element that it includes is really astounding....There is a primary this is why a ebook of this kind is way extra usefulthan an abbreviated compilation....The publication is beautiful to employees in lots of fields as a result of the great variety of the knowledge. - Philip Baumeister, Coherent Auburn crew, Auburn, California, in OPTICS AND PHOTONICS NEWS"This ebook is a vital addition to each medical reference library and to the bookshelves of all who're drawn to what's loosely known as 'the optical houses of solids."
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Extra resources for Handbook of Optical Constants of Solids, Volume 2: Volume 2
Sample text
As Spiller [18] points out, commercial computer programs may not offer any provision for setting the form of complex numbers. To obtain the correct answer, either assign negative values to the thicknesses of those films whose extinction coefficients are zero, or set k to some small value that does not significantly affect the results. Before those who use the ( n - i k ) form panic, we point out that reflectance programs that do not test complex numbers yield~the correct results most of the time.
9a for 6 - - Jr/2 are Ex = Eo cos(tot- qz) (11a) Ey = - E 0 sin(tot- qz), and the equations for 6 = + Jr/2 are Ex = Eo cos(tot- qz) (llb) Ey = Eo sin(tot- qz). Figure 2a shows a plot of the Ex and Ey components as a function of tot for 6 = - n/2, and Fig. 2b shows a similar plot for 6 = + er/2. It can be seen that when 6 = - =r/2, Ey leads Ex by n/2 (Fig. 2a), whereas when 6 = + er/2, Ey lags Ex by n/2 (Fig. 2b). 2. J iJJ wt -E6 Fig. 2. The orthogonal components of circularly polarized waves as a function of time.
The FC label attached to the reflected wave in Fig. 7a signifies the Fresnel convention. We use this label to emphasize that Er~(FC) is an arbitrarily selected vector from which one derives the Fresnel reflection coefficient. The actual reflected field may point in the same direction as the convention vector in Fig. 7a or in the opposite direction. Once the direction of E is chosen, the direction of H is determined by q x E = ~o~t0H. It must be pointed out that Fig. 7 is just a schematic representation of the actual situation.