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By G. Schmahl, D. Rudolph (auth.), Professor Dr. Günter Schmahl, Dr. Dietbert Rudolph (eds.)

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Read or Download X-Ray Microscopy: Proceedings of the International Symposium, Göttingen, Fed. Rep. of Germany, September 14–16, 1983 PDF

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For example, one of their conclusions was that it would be of no value to blaze a zone plate when "k/n ;:. 3 that doing so can actually yield efficiency gains of from 30 to BO% over the "generalized phase plate" (Case 3) - over the entire 100-600 eV range. 22) and were presented for m = 1. This was do~e to ~onserve spa~e and because the extension ~o higher zones and orders 1S eas11y made. 19), the general prof11e for the ith zone becomes (cf. 22)) hO. (r) { = 0; (ai - di (opt)) .. r hO~ (r) = t ((L2 1 + r2)1/2 - (L2 < + ai_l ..

In addition, there is the natural tendency for persons developing a particular type of light source to choose systems of units which present their source most advartageously in iabular comparisons. The use of "Peak Flux" (photons x second- x megahertz- ) is especially advantageous to sources generating high VUV outputs in very narrow wavelength intervals (i. 1) while "Average Intensity" (photons in a 1% wavelength bandwidth x seconds- 1 x milliradians- 2) would be a much more advantageous choice for sources with broad range wavelength outputs (i.

L. Csonka, and I. Lindau: "Optimization of Planar Metallic Non-Refracting Transmission-Grating Profiles for mth Order Intensity Maximization in the Soft X-Ray Range", J. Opt. Soc. Am. J. Hagemann, W. Gudat, and C. Kunz: "Optical Constants from the Far Infrared to the X-Ray Region: Mg, Al, Cu, Ag, Au, Bi, C, and A1203," Rep. No. 74/7, Deutsches Elektronen-Synchrotron, Hamburg, West Germany (1974) 50 7. Planar Techniques for Fabricating X-Ray Diffraction Gratings and Zone Plates H. I. Smith, E. H.

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