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Since the refractive index for any lens material is smaller than one (n < 1), a focusing lens needs to have a concave shape (Figure 3.4.2a). For hard X-ray energies around 20 keV, refraction is about six orders of magnitude weaker (e.g. for aluminium ( = 1.35 10 6 ) than that for visible light in glass (n 1.5). To obtain a focal distance of about 1 m for visible light, a biconvex glass lens needs to have a radius of curvature R of about 1 m. To obtain the same focal distance with an aluminium lens for X-rays (20 keV), a radius of curvature of less than R = 3 m would be required for a single biconcave lens. It is dif cult to build a lens with such a radius of curvature, in particular with a suf ciently large aperture R0 . To circumvent this dif culty, we have chosen a radius of curvature that is large enough to be manufacturable and compensate the resulting lack of refraction of a single lens by stacking N lenses behind each other as shown in Figure 3.4.2(b). This strategy has been followed by most groups that have built refractive lenses. In the X-ray range, there is no lens material that is as transparent as glass for visible light. Attenuation inside a lens is always signi cant, java code 128 reader Barcode Reader . Free Online Web Application
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