view article
Figure 2
(a) Sagittal focusing as a function of incident energy from 100 to 150 keV and the magnification at point A when [\sigma_z = \eta] is assumed and [\eta] is used. [{\rm d}\it {E/E}] is the energy spread and the magnification corresponds to [\it {q/p}]. The following parameters are used: Si 400 reflection; [\it p] = 41.2 m; [\sigma_z] = 0.06 mrad and [ \sigma_x] = 0.4 mrad. (b) Meridional focusing as a function of incident energy and the magnification at point A when equation (6)[link] is assumed and [\eta] is used. (c) Sagittal focusing as a function of incident energy and the magnification at point C when [\sigma_z = \eta] is assumed and [\eta^\prime] is used. (d) Meridional focusing as a function of incident energy and the magnification at point C when equation (6)[link] is assumed and [\eta^\prime] is used.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 5| Part 3| May 1998| Pages 687-689
https://doi.org/10.1107/S0909049597018657
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