There is a great amount of literature available indicating that membranes are inhomogeneous, complex fluids. For instance, observation of diffusion in cell membranes demonstrated confined motion of membrane constituents and even subdiffusion. In order to circumvent the small dimensions of cells leading to weak statistics when investigating the diffusion properties of single membrane components, a technique based on optical microscopy employing Langmuir monolayers as membrane model systems has been developed in our lab. In earlier work, the motion of labeled single lipids was visualized. These measurements with long observation times, thus far only possible with this method, were combined with respective Monte-Carlo simulations. We could conclude that noise can lead in general to the assumption of subdiffusion while interpreting the results of single-particle-tracking (SPT) experiments within membranes in general. Since the packing density of lipids within monolayers at the air/water interface can be changed easily, inhomogeneity with regard to the phase state can be achieved by isothermal compression to coexistence regions. Surface charged polystyrene latexes were used as model proteins diffusing in inhomogeneous monolayers as biomembrane mimics. Epifluorescence microscopy coupled to SPT revealed that domain associated, dimensionally reduced diffusion can occur in these kinds of model systems. This was caused by an attractive potential generated by condensed domains within monolayers. Monte-Carlo simulations supported this view point. Moreover, long-time simulations show that diffusion coefficients of respective particles were dependent on the strength of the attractive potential present: a behavior reflecting altered dimensionality of diffusion. The widths of those potentials were also found to be affected by the domain size of the more ordered lipid phase. In biological membrane systems, cells could utilize these physical mechanisms to adjust diffusion properties of membrane components.
Lipid membranes play a fundamental role in vital cellular functions such as signal transduction. Many of these processes rely on lateral diffusion within the membrane, generally a complex fluid containing ordered microdomains. However, little attention has been paid to the alterations in transport dynamics of a diffusing species caused by long-range interactions with membrane domains. In this paper, we address the effect of such interactions on diffusive transport by studying lateral diffusion in a phase-separated Langmuir phospholipid monolayer via single-particle tracking. We find that attractive dipole-dipole interactions between condensed phase domains and diffusing probe beads lead to transient confinement at the phase boundaries, causing a transition from two- to one-dimensional diffusion. Using Brownian dynamics simulations, the long-term diffusion constant for such a system is found to have a sensitive, Boltzmann-like, dependence on the interaction strength. In addition, this interaction strength is shown to be a strong function of the ratio of domain to particle size. As similar interactions are expected in biological membranes, the modulation of diffusive transport dynamics by varying interaction strength and/or domain size may offer cells selective spatial and temporal control over signaling processes.
We present electronic properties of a charge transfer material consisting of Manganese(ii)Phthalocyanine (MnPc) and 2,3,5,6-Tetrafluoro-7,7,8,8-tetracyanoquinodimethane (F4TCNQ), investigated by means of photoemission spectroscopy and electron energy-loss spectroscopy, as well as supporting density functional theory calculations. We report the successful formation of a bulk material characterized by a strong interaction of the molecular compounds which affects the optical properties significantly. Our investigations reveal a significant charge transfer, whereas the MnPc molecule is oxidized and F4TCNQ is reduced. The valence band data indicate a full charge transfer between the two partners. The electronic excitation spectrum reveals a relatively small energy gap of MnPc/F4TCNQ of about 0.7 eV, which is related to a charge transfer excitation.
Actin is one of the main components of the architecture of cells. Actin filaments form different polymer networks with versatile mechanical properties that depend on their spatial organization and the presence of cross-linkers. Here, we investigate the mechanical properties of actin bundles in the absence of cross-linkers. Bundles are polymerized from the surface of mDia1-coated latex beads, and deformed by manipulating both ends through attached beads held by optical tweezers, allowing us to record the applied force. Bundle properties are strikingly different from the ones of a homogeneous isotropic beam. Successive compression and extension leads to a decrease in the buckling force that we attribute to the bundle remaining slightly curved after the first deformation. Furthermore, we find that the bundle is solid, and stiff to bending, along the long axis, whereas it has a liquid and viscous behavior in the transverse direction. Interpretation of the force curves using a Maxwell visco-elastic model allows us to extract the bundle mechanical parameters and confirms that the bundle is composed of weakly coupled filaments. At short times, the bundle behaves as an elastic material, whereas at long times, filaments flow in the longitudinal direction, leading to bundle restructuring. Deviations from the model reveal a complex adaptive rheological behavior of bundles. Indeed, when allowed to anneal between phases of compression and extension, the bundle reinforces. Moreover, we find that the characteristic visco-elastic time is inversely proportional to the compression speed. Actin bundles are therefore not simple force transmitters, but instead, complex mechano-transducers that adjust their mechanics to external stimulation. In cells, where actin bundles are mechanical sensors, this property could contribute to their adaptability.
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