Scalable chemical synthesis of doped silicon nanowires for energy applications

A versatile, low-cost and easily scalable synthesis method is presented for producing silicon nanowires (SiNWs) as a pure powder. It applies air-stable diphenylsilane as a Si source and gold nanoparticles as a catalyst and takes place in a sealed reactor at 420 °C (pressure <10 bar). Micron-sized NaCl particles, acting as a sacrificial support for the catalyst particles during NW growth, can simply be removed with water during purification. This process gives access to SiNWs of precisely controlled diameters in the range of 10 ± 3 nm with a high production yield per reactor volume (1 mg cm-3). The reaction was scaled up to 500 mg of SiNWs without altering the morphology or diameter. Adding diphenylphosphine results in SiNW n-type doping as confirmed by ESR spectroscopy and EDX analyses. The measured SiNW doping level closely follows the initial dopant concentration. Doping induces both an increase in diameter and a sharp increase of electrical conductivity for P concentrations >0.4%. When used in symmetric supercapacitor devices, 1% P-doped SiNWs exhibit an areal capacity of 0.25 mF cm-2 and retention of 80% of the initial capacitance after one million cycles, demonstrating excellent cycling stability of the SiNW electrodes in the presence of organic electrolytes.

Gel phase vesicles buckle into specific shapes

Osmotic deflation of giant vesicles in the rippled gel phase P(β') gives rise to a large variety of novel faceted shapes. These shapes are also found from a numerical approach by using an elastic surface model. A shape diagram is proposed based on the model that accounts for the vesicle size and ratios of three mechanical constants: in-plane shear elasticity and compressibility (usually neglected) and out-of-plane bending of the membrane. The comparison between experimental and simulated vesicle morphologies reveals that they are governed by a typical elasticity length, of the order of 1   μm, and must be described with a large Poisson's ratio.

Influence of polyelectrolyte chemical structure on their interaction with lipid membrane of zwitterionic liposomes

In this paper we extend our previous experimental work on interaction between polyelectrolytes and liposomes. First, the adsorption of chitosan and alkylated chitosan (cationic polyelectrolytes) with different alkyl chain lengths on lipid membranes of liposomes is examined. The amount of both chitosans adsorbed remains the same even if more alkylated polysaccharide has to be added to get saturation if compared with unmodified chitosan. It is demonstrated that alkyl chains do not specifically interact with the lipid bilayer and that electrostatic interaction mechanism governs the chitosan adsorption. The difference observed between unmodified and alkylated chitosans behavior to reach the plateau can be interpreted in terms of a competition between electrostatic polyelectrolyte adsorption on lipid bilayer and hydrophobic autoassociation in solution (which depends on the alkyl chain length). Second, interaction of liposomes with hyaluronan (HA) and alkylated hyaluronan (anionic polyelectrolytes) is analyzed. The same types of results as discussed for chitosan are obtained, but in this case, autoassociation of alkylated HA only occurs in the presence of salt excess. Finally, a first positive layer of chitosan is adsorbed on the lipid membrane, followed by a second negative layer of HA at three different pHs. This kind of multilayer decoration allows the control of the net charge of the composite vesicles. A general conclusion is that whatever the pH and, consequently, the initial charge of the liposomes, chitosan adsorption gives positively charged composite systems, which upon addition of hyaluronan, give rise to negatively charged composite vesicles.

Responsive viscoelastic giant lipid vesicles filled with a poly(N-isopropylacrylamide) artificial cytoskeleton

Responsive giant lipid vesicles filled with aqueous PolyNipam sol (SFV) or gel (GFV) were prepared by ultra-violet polymerisation performed in situ. Upon crossing the lower critical transition temperature of PolyNipam, SFVs and GFVs undergo a significant change of their structural and mechanical properties or a drastic volume transition, respectively. Rheometric and micropipette experiments show that both internal viscosity of SFVs and internal shear modulus of GFVs are tunable over several orders of magnitude and lie in the range observed for living cells. Moreover, the vesicle membrane is strongly bound to the internal polymer medium, making these systems interesting for mimicking the basic mechanical behaviour of passive living cells.

Large and giant vesicles "decorated" with chitosan: effects of pH, salt or glucose stress, and surface adhesion

This paper describes the behavior of large and giant unilamellar vesicles (LUVs and GUVs, respectively) in the presence of chitosan, a positively charged polyelectrolyte. Variation of the zeta-potential of LUVs as a function of chitosan concentration is studied for two different molecular weights (MW) after a preliminary study devoted to pH and salt effects on zeta-potential in order to discriminate among the effects of protons, salt, and chitosan concentrations. The difference observed between pH and salt effects on the one hand and chitosan on the other allows us to conclude there is a strong LUV-chitosan interaction. In presence of chitosan, the zeta-potential of LUVs becomes positive and two distinct regimes of variation are suggested and interpreted as follows: a first step consists of chitosan adsorption flat on the membrane (independent of MW) followed by a possible reorganization of the polymer of higher molecular weight on the surface, giving rise to loops. Then a comparative observation of the effect of pH and salt by optical microscopy is made on naked and chitosan-decorated GUVs. Results further confirm a membrane-chitosan interaction and are interpreted in the light of the results obtained for LUVs in terms of both electrostatic and hydrophobic interaction. A large majority of decorated vesicles remain stable down to pH = 1 while in the absence of chitosan they burst quickly at pH between 2 and 3. Osmotic pressure and net charge change due to addition of HCl results in a decrease in the diameter of the decorated vesicles, which remain spherical while forming tubes of lipids. In presence of NaCl, a higher resistance of decorated vesicles is also evidenced (they are stable for NaCl concentrations up to 10-1 M while naked vesicles burst when [NaCl] is between 10-2 and 10-3 M). At higher salt concentration, aggregation of decorated vesicles occurs, which is attributed to the screening of electrostatic repulsions between vesicles covered by the positively charged chitosan. Finally, adhesion of vesicles on a positively charged surface is investigated. In absence of chitosan, the vesicles immediately burst when they come in contact with the surface. On the contrary, suspension of chitosan-vesicles remain stable down to pH = 1.5. Under gentle flow vesicles move: they do not adhere on the substrate, probably due to the repulsion between positively adsorbed charged chitosan and substrate; spherical deflation occurs, but in this case daughter vesicles are formed instead of lipid tubes.