view article
Figure 4
(a) The effect of increasing the primary beam half-height a at constant beam half-width b = 12 mm, capillary-wall thickness t = 0.01 mm and linear attenuation coefficient μ = 1.0 mm−1. (b) The effect of changing the beam half-width b and including the experimental beam profiles, all at constant t = 0.01 mm and μ = 1.0 mm−1. (c) The effect of increasing the linear attenuation coefficient μ on the angular dependence of the transmission coefficient A(2θ) at constant a = 0.1 mm, b = 12 mm and t = 0.01 mm.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 59| Part 5| October 2026|
https://doi.org/10.1107/S1600576726006837
Follow J. Appl. Cryst.
Sign up for e-alerts
E-alerts
Follow J. Appl. Cryst. on Twitter
Twitter
Follow us on facebook
Facebook
Sign up for RSS feeds
RSS