view article
Figure 9
Difference between experimental and calculated values of the phases of the fifth-order Fourier coefficients of the displacive modulation functions for model A (open circles), model Dr (filled circles) and the Aramburu et al. (2006BB1) model (diamonds). [\theta_{\rm refin}] is obtained from the refined fifth-order coefficients. [\theta_{\rm theor} = \pi-\theta_{\rm refin}^{1}-4\pi z^0(\mu)] is calculated from the phases ([\theta_{\rm refin}^{1}]) of the refined first-order Fourier coefficients of the same models according to the relation obtained for the soliton model by Aramburu et al. (2006BB1). Error bars indicate one standard uncertainty.

Journal logoSTRUCTURAL SCIENCE
CRYSTAL ENGINEERING
MATERIALS
ISSN: 2052-5206
Volume 67| Part 3| May 2011| Pages 205-217
doi:10.1107/S0108768111013814
Follow Acta Cryst. B
Sign up for e-alerts
E-alerts
Follow Acta Cryst. on Twitter
Twitter
Follow us on facebook
Facebook
Sign up for RSS feeds
RSS