view article
Figure 10
The double-diffracted beam intensity distribution on the focusing plane in a RDL with a silicon lens. Shown are the cases corresponding to magnifications M = 1 (a), M = 1.5 (b), M = 0.5 (c). The beam falls at the Bragg-corrected angle corresponding to the wave with [\Delta\lambda/\lambda_{\rm{m}}] = 0. Absorption in the lens is taken into account. Numerical integration by formula (79)[link]. Point source.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 17| Part 3| March 2010| Pages 332-347
doi:10.1107/S0909049510003754
Follow J. Synchrotron Rad.
Sign up for e-alerts
E-alerts
Follow J. Synchrotron Rad. on Twitter
Twitter
Follow us on facebook
Facebook
Sign up for RSS feeds
RSS