view article
Figure 2
An electron passes through a bending magnet and its narrow synchrotron `cone' of width ∼2/γ sweeps through a point-like detector. (a) When the detection starts, the electron–detector line of sight is at an angle θ = θM ≃ 1/γ from the longitudinal direction. Then (b) θ decreases to zero, and afterwards (c) it increases again to θM.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 25| Part 4| July 2018| Pages 1271-1276
https://doi.org/10.1107/S1600577518005441
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