Jordi Ignés-Mullol

Shear-induced molecular precession in a hexatic Langmuir monolayer.

Liquid crystalline behaviour is generally limited to a select group of specially designed bulk substances. By contrast, it is a common feature of simple molecular monolayers and other quasi-two-dimensional systems, which often possess a type of in-plane ordering that results from unbinding of dislocations—a ‘hexatic’ liquid crystalline phase. The flow of monolayers is closely related to molecular transport in biological membranes, affects foam and emulsion stability and is relevant to microfluidics research. For liquid crystalline phases, it is important to understand the coupling of the molecular orientation to the flow. Orientationally ordered (nematic) phases in bulk liquid crystals exhibit ‘shear aligning’ or ‘tumbling’ behaviour under shear, and are described quantitatively by Leslie–Ericksen theory. For hexatic monolayers, the effects of flow have been inferred from textures of Langmuir–Blodgett films and directly observed at the macroscopic level. However, there is no accepted model of hexatic flow at the molecular level. Here we report observations of a hexatic Langmuir monolayer that reveal continuous, shear-induced molecular precession, interrupted by occasional jump discontinuities. Although superficially similar to tumbling in a bulk nematic phase, the kinematic details are quite different and provide a possible mechanism for domain coarsening and eventual molecular alignment in monolayers. We explain the precession and jumps within a quantitative framework that involves coupling of molecular orientation to the local molecular hexatic ‘lattice’, which is continuously deformed by shear.

Control of active liquid crystals with a magnetic field

Significance Active liquid crystals are aqueous in vitro suspensions of cytoskeletal proteins that self-assemble into elongated fibers and develop sustained flows at the continuous expense of ATP. When they condense on soft interfaces, the aligned fibers organize into nonequilibrium analogs of passive liquid crystals. However, proteins do not respond to external electromagnetic fields, unlike liquid crystals, which are readily reconfigured inside devices. We demonstrate a reversible and biocompatible experimental protocol to align an active liquid crystal with a uniform magnetic field, allowing the transition between turbulent and laminar flow regimes. The active liquid crystal senses the interfacial viscous anisotropy of a lamellar hydrophobic liquid crystal, not unlike the adaptation of cells to the mechanical features of their environment. Living cells sense the mechanical features of their environment and adapt to it by actively remodeling their peripheral network of filamentary proteins, known as cortical cytoskeleton. By mimicking this principle, we demonstrate an effective control strategy for a microtubule-based active nematic in contact with a hydrophobic thermotropic liquid crystal. By using well-established protocols for the orientation of liquid crystals with a uniform magnetic field, and through the mediation of anisotropic shear stresses, the active nematic reversibly self-assembles with aligned flows and textures that feature orientational order at the millimeter scale. The turbulent flow, characteristic of active nematics, is in this way regularized into a laminar flow with periodic velocity oscillations. Once patterned, the microtubule assembly reveals its intrinsic length and time scales, which we correlate with the activity of motor proteins, as predicted by existing theories of active nematics. The demonstrated commanding strategy should be compatible with other viable active biomaterials at interfaces, and we envision its use to probe the mechanics of the intracellular matrix.Motor-proteins are responsible for transport inside cells. Harnessing their activity is key towards developing new nano-technologies, or functional biomaterials. Cytoskeleton-like networks, recently tailored in vitro, result from the self-assembly of subcellular autonomous units. Taming this biological activity bottom-up may thus require molecular level alterations compromising protein integrity. Taking a top-down perspective, here we prove that the seemingly chaotic flows of a tubulin-kinesin active gel can be forced to adopt well-defined spatial directions by tuning the anisotropic viscosity of a contacting lamellar oil. Different configurations of the active material are realized, when the passive oil is either unforced or commanded by a magnetic field. The inherent instability of the extensile active fluid is thus spatially regularized, leading to organized flow patterns, endowed with characteristic length and time scales. Our finding paves the way for designing hybrid active/passive systems where ATP-driven dynamics can be externally conditioned.

Reconfigurable Swarms of Nematic Colloids Controlled by Photoactivated Surface Patterns

Different phoretic driving mechanisms have been proposed for the transport of solid or liquid microscopic inclusions in integrated chemical processes. It is now shown that a substrate that was chemically modified with photosensitive self-assembled monolayers enables the direct control of the assembly and transport of large ensembles of micrometer-sized particles and drops that were dispersed in a thin layer of anisotropic fluid. This strategy separates particle driving, which was realized by AC electrophoresis, and steering, which was achieved by elastic modulation of the nematic host fluid. Inclusions respond individually or in collective modes following arbitrary reconfigurable paths that were imprinted by irradiation with UV or blue light. Relying solely on generic material properties, the proposed procedure is versatile enough for the development of applications that involve either inanimate or living materials.

Stirring competes with chemical induction in chiral selection of soft matter aggregates

Chirality, the absence of mirror symmetry, can be equally invoked in relation to physical forces and chemical induction processes, yet a competition between these two types of influence is rarely reported. Here we present a self-assembled soft matter system in which chiral selection is controlled by the combined independent action of a chiral dopant and vortical stirring, which are arbitrarily coupled, either constructively or destructively. In the latter case, perfect compensation, that is, absence of a net chiral effect, is realized. The induced enantiomorphic excess is measured in terms of the statistical imbalance of an ensemble of submillimetre domains, where achiral molecules self-assemble with a well-defined orientational chirality that is unambiguously resolved using optical microscopy. The possibility of combining top-down and bottom-up strategies to induce a chiral predominance in a supramolecular system of achiral components should be recognized as a new twist in the process of chiral recognition, selection and control.

Acyl chain differences in phosphatidylethanolamine determine domain formation and LacY distribution in biomimetic model membranes.

Phosphatidylethanolamine (PE) and phosphatidylglycerol (PG) are the two main components of the inner membrane of Escherichia coli. It is well-known that inner membrane contains phospholipids with a nearly constant polar headgroup composition. However, bacteria can regulate the degree of unsaturation of the acyl chains in order to adapt to different external stimuli. Studies on model membranes of mixtures of PE and PG, mimicking the proportions found in E. coli, can provide essential information on the phospholipid organization in biological membranes and may help in the understanding of membrane proteins activity, such as lactose permease (LacY) of E. coli. In this work we have studied how different phosphatidylethanolamines differing in acyl chain saturation influence the formation of laterally segregated domains. Three different phospholipid systems were studied: DOPE:POPG, POPE:POPG, and DPPE:POPG at molar ratios of 3:1. Lipid mixtures were analyzed at 24 and 37 °C through three different model membranes: monolayers, liposomes, and supported lipid bilayers (SLBs). Data from three different techniques, Langmuir isotherms, Laurdan generalized polarization, and atomic force microscopy (AFM), evidenced that only the DPPE:POPG system exhibited coexistence between gel (L(β)) and fluid (L(α)) phases at both 24 and 37 °C . In the POPE:POPG system the L(β)/L(α) coexistence appears at 27 °C. Therefore, in order to investigate the distribution of LacY among phospholipid phases, we have used AFM to explore the distribution of LacY in SLBs of the three phospholipid systems at 27 °C, where the DOPE:POPG is in L(α) phase and POPE:POPG and DPPE:POPG exhibit L(β)/L(α) coexistence. The results demonstrate the preferential insertion of LacY in fluid phase.

AC electrophoresis of microdroplets in anisotropic liquids: transport, assembling and reaction

We describe the realization and controlled transport of water-based microreactors dispersed in a nematic liquid crystal and transported by application of an alternating electric field through the mechanism of induced charge electrophoresis. We characterize the propulsion speed of these microreactors in terms of droplet size, strength and frequency of the applied field and show how to use them to transport microscale colloidal cargoes and coalesce water miscible chemicals. Controlled motion of microdoplets in anisotropic fluids is a rich field of research which unveils new perspectives in the transport of water miscible chemicals or drugs.

Modifying surface properties of diamond-like carbon films via nanotexturing

Diamond-like amorphous carbon (DLC) films have been grown by pulsed-dc plasma-enhanced chemical vapour deposition on silicon wafers, which were previously patterned by means of colloidal lithography. The substrate conditioning comprised two steps: first, deposition of a self-assembled monolayer of silica sub-micrometre spheres (~300 nm) on monocrystalline silicon (~5 cm2) by Langmuir–Blodgett technique, which acted as lithography template; second, substrate patterning via ion beam etching (argon) of the colloid samples (550 eV) at different incidence angles. The plasma deposition of a DLC thin film on the nanotextured substrates resulted in hard coatings with distinctly different surface properties compared with planar DLC. Also, in-plane anisotropy was generated depending on the etching angle. The samples were morphologically characterized by scanning electron microscopy and atomic force microscopy. The anisotropy introduced by the texture was evidenced in the surface properties, as shown by the directional dependences of wettability (water contact angle) and friction coefficient. The latter was measured using a nanotribometer and a lateral force microscope. These two techniques showed how the nanopatterns influenced the tribological properties at different scales of load and contact area. This fabrication technique finds applications in the industry of microelectromechanical systems, anisotropic tribological coatings, nanoimprint lithography, microfluidics, photonic crystals, and patterned surfaces for biomedicine.

FORMATION OF DISCLINATION LINES NEAR A FREE NEMATIC INTERFACE

We have studied the nucleation and the physical properties of a -1/2 wedge disclination line near the free surface of a confined nematic liquid crystal. The position of the disclination line has been related to the material parameters (elastic constants, anchoring energy and favored anchoring angle of the molecules at the free surface). The use of a planar model for the structure of the director field (whose predictions have been contrasted to those of a fully three-dimensional model) has allowed us to relate the experimentally observed position of the disclination line to the relevant properties of the liquid crystals. In particular, we have been able to observe the collapse of the disclination line due to a temperature-induced anchoring angle transition, which has allowed us to rule out the presence of a real disclination line near the nematic/isotropic front in directional growth experiments. 61.30.Jf,this http URL

Continuous Rotation of Achiral Nematic Liquid Crystal Droplets Driven by Heat Flux

Suspended droplets of cholesteric (chiral nematic) liquid crystals spontaneously rotate in the presence of a heat flux due to a temperature gradient, a phenomenon known as the Lehmann effect. So far, it is not clear whether this effect is due to the chirality of the phase and the molecules or only to the chirality of the director field. Here, we report the continuous rotation in a temperature gradient of nematic droplets of a lyotropic chromonic liquid crystal featuring a twisted bipolar configuration. The achiral nature of the molecular components leads to a random handedness of the spontaneous twist, resulting in the coexistence of droplets rotating in the two senses, with speeds proportional to the temperature gradient and inversely proportional to the droplet radius. This result shows that a macroscopic twist of the director field is sufficient to induce a rotation of the droplets, and that the phase and the molecules do not need to be chiral. This suggests that one can also explain the Lehmann rotation in cholesteric liquid crystals without introducing the Leslie thermomechanical coupling-only present in chiral mesophases. An explanation based on the Akopyan and Zeldovich theory of thermomechanical effects in nematics is proposed and discussed.

Role of anisotropy in electrodynamically induced colloidal aggregates.

We investigate the assembly of spherical and anisotropic colloidal particles with the shape of peanuts when subjected to an external alternating electric field. By varying the strength and frequency of the applied field, we observe that both types of particles form clusters at low frequencies due to attractive electrohydrodynamic interactions or disperse into a liquidlike phase at high frequencies due to repulsive dipolar interactions. We characterize the observed structures via pair correlation functions and radius of gyration, and observe a clear difference in the ordering process between the isotropic and anisotropic colloids. Further on, we interpret the cluster formation kinetics in terms of dynamic scaling theory, and observe a faster aggregation of the anisotropic colloids with respect to the isotropic ones.