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. 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

Fig. 7.

Fig. 7

Red: tWAXS intensity in the qz direction along Bragg red I in the ripple phase (red) showing the breaking of the (2,0) and (−2,0) symmetry. Black: (±2,0) gel phase with the qz = 0 at the maximum intensity scaled and displaced for comparison to the ripple width. The arrow shows the width Δqz used in the text and Table 1.