view article
Figure 1
Overview of the experimental design and the technical setup at the Australian Synchrotron Far-IR/THz beamline. (a) Schematic representation of AuSi NS localization in PC 12. The SS THz exposed PC 12 samples were analysed for AuSi NPs following a 10 min exposure. (b) BEP at the Australian Synchrotron Far-IR/THz beamline, with the inset showing the beam axis in red; the beam is present within a 19 mm diameter (blue arrow) from the inner edge to the beam axis. The PC 12 cell suspension was placed on a polyethyl­ene window (red arrow) using an O-ring in the presence of the beam. (c) The spectrum of the intensity of the Australian Synchrotron THz beamline as shown by the resident Si bolometer; intensity is presented in arbitrary units, with a logarithmic scale for the THz frequencies (Vilagosh et al., 2022BB31). (d) Depth-dependent absorption pattern of the Australian Synchrotron THz beam. The two variables share an exponential relationship where the absorption of the beam decreases as the depth of the sample increases.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 30| Part 4| July 2023| Pages 780-787
https://doi.org/10.1107/S1600577523004228
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