view article
Figure 2
Upper panel: Fe K-edge irreducible [\gamma^{(2)}] and [\gamma^{(3)}] [[\eta^{(3)}=\gamma^{(2)}_{\rm L}+\gamma^{(3)}]] MS signals calculated for [\theta=180]° (upper) and 120° (lower) Fe—O—O configurations. Lower panel: average amplitude of the [\gamma^{(2)}_{\rm L}] (dots, Fe—O), [\gamma^{(3)}] (solid) and [\eta^{(3)}] (squares) MS signals as a function of the bond angle [\theta].

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 10| Part 1| December 2003| Pages 46-50
doi:10.1107/S0909049502017193
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