view article
Figure 3
From proxies to a direct measure of stress. Three ways of probing the individual bubble elastic stress tensor: (a) strain tensor [{\bf{U}}_{\rm{S}}] derived from the bubble shape tensor S, i.e. from its shape anisotropy [see equation (3)[link]], (b) strain tensor [{\bf{U}}_{\rm{M}}] derived from the bubble texture tensor M, i.e. from the anisotropy of the network of vector links to neighboring bubbles [see equation (4)[link]], (c) direct measure of the elastic stress tensor σ integrated on the full bubble interface using equation (5)[link].

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 32| Part 5| September 2025| Pages 1370-1377
https://doi.org/10.1107/S1600577525006629
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