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. Author manuscript; available in PMC: 2012 May 18.
Published in final edited form as: J Am Chem Soc. 2011 Apr 26;133(19):7585–7595. doi: 10.1021/ja202082c

Figure 8.

Figure 8

(A) Synchrotron SAXS profiles of CL-sDNA complexes containing 11 bp DNA with 2-T non-sticky overhangs (11bp DNA-2T) as a function of neutral lipid mole fraction (ΦNL). The (00L) diffraction peaks result from the multilamellar structure of the complexes. Lines point to relatively sharp sDNA–sDNA correlation peaks indicative of the new type of columnar nematic phase (Fig. 1C) as described in the text. Arrows point to broad sDNA peaks characteristic of the isotropic phase. (B–E) Plots of the interlayer spacing d (B), the average spacing between sDNA molecules dDNA (C), the correlation length LC (D), and LC in units of dDNA (E) as a function of ΦNL for CL–sDNA complexes containing 11bp DNA-2T (open circles) and for comparison 11bp DNA-5T (open squares) and 11bp DNA-10T (open triangles). The parameters result from line shape fits of the q002 and qsDNA peaks in the SAXS profiles of the corresponding complexes with a double Lorentzian. The observed values of LC (D) and LC/dDNA (E) for 11bp DNA-2T show a highly correlated nematic phase with LC/dDNA ranging between six and ten, in contrast to the isotropic phase with LC/dDNA < 1 observed for 11bp DNA-10T and 11bp DNA-5T. This new phase undergoes a transition to the isotropic phase for ΦNL > 0.5 (where LC/dDNA decreases to ≈1). The building blocks of this highly correlated nematic phase (labeled columnar nematic, NC) are 1D stacks of 11bp DNA-2T rods that result from the onset of strong sDNA end-to-end interactions. Applying Onsager's criterion to this phase gives an estimate of the stack length as on average 4 rods, as shown in Fig. 1C.