Structural Properties of the Sliding Columnar Phase in Layered Liquid Crystalline Systems

Under appropriate conditions, mixtures of cationic and neutral lipids and DNA in water condense into complexes in which DNA strands form local 2D smectic lattices intercalated between lipid bilayer membranes in a lamellar stack. These lamellar DNA-cationic-lipid complexes can in principle exhibit a variety of equilibrium phases, including a columnar phase in which parallel DNA strands from a 2D lattice, a nematic lamellar phase in which DNA strands align along a common direction but exhibit no long-range positional order, and a possible new intermediate phase, the sliding columnar (SC) phase, characterized by a vanishing shear modulus for relative displacement of DNA lattices but a nonvanishing modulus for compressing these lattices. We develop a model capable of describing all phases and transitions among them and use it to calculate structural properties of the sliding columnar phase. We calculate displacement and density correlation functions and x-ray scattering intensities in this phase and show, in particular, that density correlations within a layer have an unusual $\exp(- {\rm const.} \ln^2 r)$ dependence on separation r. We investigate the stability of the SC phase with respect to shear couplings leading to the columnar phase and dislocation unbinding leading to the lamellar nematic phase. For models with interactions only between nearest neighbor planes, we conclude that the SC phase is not thermodynamically stable. Correlation functions in the nematic lamellar phase, however, exhibit SC behavior over a range of length scalesComment: 28 pages, 4 figure

Thermotropic structural changes of saturated-cationic-lipid–DNA complexes

We investigated the thermotropic behavior of fully hydrated saturated cationic lipid mixture of DMPC/DMTAP (dimyristoylphosphatidyl-choline/dimyristoyl-trimethyl-am monium propane) complexed with DNA. Using simultaneous small- and wide-angle X-ray scattering, we found two condensed lamellar phases, a fluid $\rm L^c_\alpha$- and a gel-state $\rm L^c_{\beta'}$-phase. The chain-melting transition was accompanied by a decrease in the bilayer thickness and an expansion of the intercalated one-dimensional DNA rod lattice. The interaxial DNA-DNA spacings are quantitatively described by conservation of local volume fractions for both phases in excess water. The line broadening of the wide-angle scattering exhibited a systematic variation in the hydrocarbon chain tilt as a function of the cationic lipid molar fraction

Hydrophilic/Hydrophobic Balance Determines Morphology of Glycolipids with Oligolactose Headgroups

The morphology of synthetic glycolipids with lactose oligomers (Lac N, the number of lactose units, N = 1, 2, 3) was studied in lamellar phase. By a systematic combination of differential scanning calorimetry and small- and wide-angle x-ray scattering experiments, the effects of hydrophilic/hydrophobic balance on their thermotropic phase behaviors were discussed. The dispersion of Lac 1 exhibited a crystalline-fluid phase transition, dominated by the strong van der Waals interaction between dihexadecyl chains. In the case of Lac 2, the hydrophilic/hydrophobic balance between the headgroup and the alkyl chains is shifted to the hydrophilic side, resulting in a gel-fluid phase transition with a decreased transition temperature and phase transition enthalpy. Different from the first two systems, the differential scanning calorimetry trace of Lac 3 showed much less remarkable peaks. The small- and wide-angle x-ray diffraction patterns did not reveal any transition in the chain ordering, suggesting that the correlation between the hexasaccharide headgroups is so strong that the melting of the alkyl chains was not allowed. Such dominant effects of the hydrophilic/hydrophobic balance on the morphology of Lac N lipids can be attributed to the small sterical mismatch between the alkyl chains and the linear, cylindrical oligolactose groups