view article
Figure 11
Error diagrams for type I spectrometers constructed using silver (top panel), tungsten (middle panel) and gold (bottom panel). The discontinuity in the top panel is due to the silver K-edge. Discontinuities in the W and Au data are due to L-edge effects. Of these elements, only silver is able to provide good energy measurements out to 60 keV. Au (K-edge 80 keV) and W (K-edge 69 keV) could be employed to good effect in spectrometers working up to 100 keV. Simulations all assume that I0 is 10000. Silver simulation consists of 30 (filled squares), 60 (open squares), 90 (filled diamonds), 120 (open diamonds), 150 (filled circles), 180 (open circles) and 210 µm (crosses) foil thickness. Tungsten and gold simulations consist of 15 (filled squares), 25 (open squares), 35 (filled diamonds), 45 (open diamonds), 55 (filled circles), 65 (open circles) and 75 µm (crosses) foils.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 12| Part 5| August 2005| Pages 618-625
doi:10.1107/S0909049505022600
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