Specific adsorption of functionalized colloids at the surface of living cells: a quantitative kinetic analysis of the receptor-mediated binding.

This paper presents a statistical experimental study of the adsorption of colloids onto the plasma membrane of living cells mediated by specific ligand-receptor interactions. The colloids consist of lipid multilamellar liposomes (spherulites) functionalized by Shiga toxin B-subunit (STxB), while cells are cervix carcinoma epithelial cells expressing the Shiga toxin receptor, the glycolipid globotriaosyl ceramide (Gb3). The specificity of the colloid adsorption is demonstrated using both confocal microscopy and flow cytometry, while a thorough cytometry study on living cells allows characterizing the kinetics of this specific adsorption. The final number of bound colloids and the characteristic adsorption time are shown to depend on bulk concentration, as expected for a thermodynamic equilibrium. However, the colloids appear to be irreversibly attached to the membrane. We interpret this apparent irreversibility as the result of a progressive recruitment of receptors. The methodology used here, whereby microscopic mechanisms are deduced from direct quantitative measurements on living cells, might allow the optimization of drug delivery systems or the quantification of virus infectivity.

Key role of receptor density in colloid/cell specific interaction: a quantitative biomimetic study on giant vesicles.

This paper presents an experimental study of the adsorption of colloids on model membranes mediated by specific ligand-receptor interactions. The colloids consist of lipid multilamellar liposomes (spherulites) functionalized with the B-subunit of Shiga Toxin (STxB), while the membranes are lipid Giant Unilamellar Vesicles (GUV) containing STxB lipid receptor, Globotriaosylceramide (Gb3). Through confocal microscopy and flow cytometry, we show the specificity of the adsorption. Moreover, we show that flow cytometry can be used to efficiently quantify the kinetics of colloid adsorption on GUVs with very good statistics. By varying the bulk colloid concentration and receptor density in the membrane, we point out the existence of an optimum Gb3 density for adsorption. We propose that this optimum corresponds to a transition between reversible colloid adsorption at low Gb3 density and irreversible adsorption, and likely spherulite fusion, at high density. We compare our results both to STxB-colloids adhering on living cells and to free STxB proteins interacting with GUVs containing Gb3. This biomimetic system could be used for a quantitative evaluation of the early stage of virus infection or drug delivery.

Confined diffusion of hydrophilic probes inserted in lyotropic lamellar phases.

The dynamic behaviour of three hydrophilic probes (two dyes and one fluorescently-labelled protein) inserted in the water layers of lyotropic lamellar phases has been studied by confocal fluorescence recovery experiments. Two different, ionic (AOT/NaCl/ H(2)O and non-ionic ( C(12)E(5) /hexanol/ H(2)O host systems were studied. The confinement effect has been carefully monitored using the swelling properties of the lamellar phases. In all cases, we measure the evolution of the probe diffusion coefficient in the layer plane D ( perpendicular) versus the separation between the membranes d(w). Depending on the composition of the lamellar phase, this distance can be continuously adjusted from 500A to about 20A. For all systems, we observe a first regime, called dilute regime, where the diffusion coefficient decreases almost linearly with 1/d (w) . In this regime, the Faxén theory for the friction coefficient of a spherical particle symmetrically dragged between two rigid walls can largely explain our results. More unexpectedly, when the membranes are non-ionic, and also quite flexible ( C(12)E(5) /hexanol in water), we observe the existence of a second, concentrated (or confined) regime, where the diffusion coefficient is nearly constant and different from zero for membrane separations smaller than the particle size. This new regime can be heuristically explained by simple arguments taking into account the membrane fluidity.

Stability of thin nematic films. Commentary on "Morphology and structure of thin liquid-crystalline films at nematic-isotropic transition" by P. Ziherl and S. Zumer.

We discuss the peculiarity of thin nematic films on solid substrates with a free surface, underlining the differences with what is usually seen in dewetting. We review the thermodynamic basis of the coupled phase/thickness separation that has previously been shown experimentally. We give new experimental evidences for the origin of the coupling force chosen in our previous theoretical model. This additional information contributes to the discussion raised by the article of Ziherl and Zumer in this issue.

Binary separation in very thin nematic films: thickness and phase coexistence.

The behavior as a function of temperature of very thin films (10 to 200 nm) of pentylcyanobiphenyl on silicon substrates is reported. In the vicinity of the nematic-isotropic transition we observe a coexistence of two regions of different thicknesses: thick regions are in the nematic state while thin ones are in the isotropic state. Moreover, the transition temperature is shifted downward following a 1/h(2) law ( h is the film thickness). Microscope observations and small-angle x-ray scattering allowed us to draw a phase diagram which is explained in terms of a binary first-order phase transition where thickness plays the role of an order parameter.