. Author manuscript; available in PMC: 2016 Feb 7.

Published in final edited form as: Soft Matter. 2015 Feb 7;11(5):918–926. doi: 10.1039/c4sm02335h

Table 1.

Wide angle quantities in Å⁻¹ for the Bragg rods indicated by arrows I and II in Fig. 3 are given in the first two rows. The third row is for a broad underlying intensity not visible in Fig. 3. The remaining rows give results for the gel and fluid phases. The gel I width 0:014^a is the limit of our instrumental resolution. Δq_r is FWHM. Δq_z is shown in Fig. 7.

Rods	q	q_r	q_z	Δ q_r	Δ q_z
ripple I	1.49	1.48	0.20	0.025	0.4
ripple II	1.46	1.46	0.12	0.025	0.4
broader	1.47	1.46		0.140
gel I	1.48	1.48	0	0.014^a	0.4
gel II	1.54	1.36	0.72
fluid	1.41			0.29