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Formation of Optical Images by X-Rays

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1948

Year

TLDR

Several conceivable methods for the formation of optical images by x‑rays are considered, and a method employing concave mirrors is adopted as the most promising. A concave spherical mirror at grazing incidence images a point into a line with focal length f = Ri/2, but peripheral rays suffer an aberration (S ≈ 1.5 M r²/R), and extended images can be obtained by reflecting the radiation from two concave mirrors in series. The system can theoretically resolve point objects separated by about 70 Å regardless of wavelength, and sample results confirm this capability.

Abstract

Several conceivable methods for the formation of optical images by x-rays are considered, and a method employing concave mirrors is adopted as the most promising. A concave spherical mirror receiving radiation at grazing incidence (a necessary arrangement with x-rays) images a point into a line in accordance with a focal length f=Ri/2 where R is the radius of curvature and i the grazing angle. The image is subject to an aberration such that a ray reflected at the periphery of the mirror misses the focal point of central rays by a distance given approximately by S=1.5Mr2/R, where M is the magnification of the image and r is the radius of the mirror face. The theoretically possible resolving power is such as to resolve point objects separated by about 70A, a limit which is independent of the wave-length used. Point images of points and therefore extended images of extended objects may be produced by causing the radiation to reflect from two concave mirrors in series. Sample results are presented.

References

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