Transmembrane Signaling with Lipid‐Bilayer Assemblies as a Platform for Channel‐Based Biosensing

Artificial and natural lipid membranes that elicit transmembrane signaling is are useful as a platform for channel‐based biosensing. In this account we summarize our research on the design of transmembrane signaling associated with lipid bilayer membranes containing nanopore‐forming compounds. Channel‐forming compounds, such as receptor ion‐channels, channel‐forming peptides and synthetic channels, are embedded in planar and spherical bilayer lipid membranes to develop highly sensitive and selective biosensing methods for a variety of analytes. The membrane‐bound receptor approach is useful for introducing receptor sites on both planar and spherical bilayer lipid membranes. Natural receptors in biomembranes are also used for designing of biosensing methods.     

L‐Tryptophan‐Induced Electron Transport across Supported Lipid Bilayers: an Alkyl‐Chain Tilt‐Angle,and Bilayer‐Symmetry Dependence

Molecular orientation‐dependent electron transport across supported 1,2‐dipalmitoyl‐sn‐glycero‐3‐phosphocholine (DPPC) lipid bilayers (SLBs) on semiconducting indium tin oxide (ITO) is reported with an aim towards potential nanobiotechnological applications. A bifunctional strategy is adopted to form symmetric and asymmetric bilayers of DPPC that interact with L ‐tryptophan, and are analyzed by surface manometry and atomic force microscopy. Polarization‐dependent real‐time Fourier transform infrared reflection absorption spectroscopy (FT‐IRRAS) analysis of these SLBs reveals electrostatic, hydrogen‐bonding, and cation–π interactions between the polar head groups of the lipid and the indole side chains. Consequently, a molecular tilt arises from the effective interface dipole, facilitating electron transport across the ITO‐anchored SLBs in the presence of an internal Fe(CN)₆^4?/3? redox probe. The incorporation of tryptophan enhances the voltammetric features of the SLBs. The estimated electron‐transfer rate constants for symmetric and asymmetric bilayers (k_s=2.0×10^?2 and 2.8×10^?2 s^?1) across the two‐dimensional (2D) ordered DPPC/tryptophan SLBs are higher compared to pure DPPC SLBs (k_s=3.2×10^?3 and 3.9×10^?3 s^?1). In addition, they are molecular tilt‐dependent, as it is the case with the standard apparent rate constants ${k_{{\rm{app}}}^0 }$ , estimated from electrochemical impedance spectroscopy and bipotentiostatic experiments with a Pt ultramicroelectrode. Lower magnitudes of k_s and ${k_{{\rm{app}}}^0 }$ imply that electrochemical reactions across the ITO–SLB electrodes are kinetically limited and consequently governed by electron tunneling across the SLBs. Standard theoretical rate constants ${\left( {k_{{\rm{th}}}^0 } \right)}$ accrued upon electron tunneling comply with the potential‐independent electron‐tunneling coefficient β=0.15 Å^?1. Insulator–semiconductor transitions moving from a liquid‐expanded to a condensed 2D‐phase state of the SLBs are noted, adding a new dimension to their transport behavior. These results highlight the role of tryptophan in expediting electron transfer across lipid bilayer membranes in a cellular environment and can provide potential clues towards patterned lipid nanocomposites and devices.     

Dark‐Field‐Based Observation of Single‐Nanoparticle Dynamics on a Supported Lipid Bilayer for In Situ Analysis of Interacting Molecules and Nanoparticles

Observation of single plasmonic nanoparticles in reconstituted biological systems allows us to obtain snapshots of dynamic processes between molecules and nanoparticles with unprecedented spatiotemporal resolution and single‐molecule/single‐particle‐level data acquisition. This Concept is intended to introduce nanoparticle‐tethered supported lipid bilayer platforms that allow for the dynamic confinement of nanoparticles on a two‐dimensional fluidic surface. The dark‐field‐based long‐term, stable, real‐time observation of freely diffusing plasmonic nanoparticles on a lipid bilayer enables one to extract a broad range of information about interparticle and molecular interactions throughout the entire reaction period. Herein, we highlight important developments in this context to provide ideas on how molecular interactions can be interpreted by monitoring dynamic behaviors and optical signals of laterally mobile nanoparticles.     

Transport of Cesium Ion Across a Bilayer Lipid Membrane and Its Facilitation in the Presence of Iodide Ion

The ion transport current was clearly observed across a bilayer lipid membrane (BLM) between two aqueous phases (W1, W2) containing 0.1 M CsCl. This indicates that Cs⁺ can spontaneously penetrate the BLM in the absence of any kind of transporter. In addition, the current density at a given potential between W1 and W2 increased using I^? instead of Cl^? as the counter ion. Our results strongly suggest that the cell membrane transport is partially responsible for the internal exposure of ¹³⁴Cs and ¹³⁷Cs.     

Unique Vibrational Features as a Direct Probe of Specific Antigen–Antibody Recognition at the Surface of a Solid‐Supported Hybrid Lipid Bilayer

Here, we demonstrate how sum frequency generation (SFG), a vibrational spectroscopy based on a nonlinear three‐photon mixing process, may provide a direct and unique fingerprint of bio‐recognition; This latter can be detected with an intrinsically discriminating unspecific adsorption, thanks to the high sensitivity of the second‐order nonlinear optical (NLO) response to preferential molecular orientation and symmetry properties. As a proof of concept, we have detected the biological event at the solid/liquid interface of a model bio‐active antigen platform, based on a solid‐supported hybrid lipid bilayer (ss‐HLB) of a 2,4‐dinitrophenyl (DNP) lipid, towards a monoclonal mouse anti‐DNP complementary antibody.     

Mechanisms of Biological Ion Transport — Carriers,Channels, and Pumps in Artificial Lipid Membranes

The cell membrane contains specific systems for passive and active transport of ions between the cytoplasm and the extracellular medium. For a number of small and medium-sized transport molecules like valinomycin and gramicidin A, extensive structural and kinetic data are available and it is possible in these cases to understand the transport function on the basis of their molecular structure. Incorporation into artificial bimolecular lipid membranes opens up the possibility of studying the kinetic properties of biological transport systems in detail.     

Artificial Formation and Tuning of Glycoprotein Networks on Live Cell Membranes: A Single‐Molecule Tracking Study

We present a method to artificially induce network formation of membrane glycoproteins and show the precise tuning of their interconnection on living cells. For this, membrane glycans are first metabolically labeled with azido sugars and then tagged with biotin by copper‐free click chemistry. Finally, these biotin‐tagged membrane proteins are interconnected with streptavidin (SA) to form an artificial protein network in analogy to a lectin‐induced lattice. The degree of network formation can be controlled by the concentration of SA, its valency, and the concentration of biotin on membrane proteins. This was verified by investigation of the spatiotemporal dynamics of the SA‐protein networks employing single‐molecule tracking. It was also proven that this network formation strongly influences the biologically relevant process of endocytosis as it is known from natural lattices on the cell surface.     

Self‐Assembled Aggregates and Molecular Bilayer Films of a Double‐Chain Fullerene Lipid: Structure and Electrochemistry

The self‐aggregation behavior of C₆₀ fullerenes that bear two octadecyl chains (lipid 1 ) as well as the structures and electrochemical properties of cast films of 1 are described. We also examined the self‐aggregation behavior in organic solvents of three previously reported compounds: C₆₀ with three each of hexadecyl (lipid 2 ), tetradecyl (lipid 3 ), or dodecyl (lipid 4 ) chains. The fullerene lipids in alcohols spontaneously formed spherical aggregates, whose diameters are related to the alkyl‐chain lengths, concentrations of the fullerene lipids, and the solvent polarity. The morphologies of the aggregates showed temperature dependence. Cast films of 1 formed multimolecular bilayer structures that undergo a phase transition typical of lipid bilayer membranes. The electrochemistry of cast films of 1 on an electrode in aqueous medium exhibits temperature dependence.     

Single Oxygen‐Atom Insertion into PB Bonds: On‐ and Off‐Metal Transformation of a Borylphosphine into a Borylphosphinite

An oxygen atom is selectively inserted into the P?B bond of a borylphosphine ( L₁ ) by reaction with Me₃NO to afford the corresponding borylphosphinite ( L₂ ). This transformation can also be effected when L₁ is coordinated to rhodium. The ν(CO) values for trans‐[RhCl(CO)(L)₂] reveal very different electronic properties for coordinated L₁ and L₂ which translate into the strikingly different performances of the complexes [RhCl(L)(cod)] (L= L₁ or L₂ , cod=1,5‐cyclooctadiene) in hydrosilylation and hydroboration catalysis.     

Reversible 1,1‐Hydroboration: Boryl Insertion into a CN Bond and Competitive Elimination of HBR2 or RH

Boranes with the general formula of HBR₂ have been found to undergo a facile 1,1‐hydroboration reaction with pyrido[1,2‐a]isoindole ( A ), resulting in insertion of a BR₂ unit into a C? N bond and the formation of a variety of BN heterocycles. Investigation on the thermal reactivity of the BN heterocycles revealed that these molecules have two distinct and competitive thermal elimination pathways: HBR₂ elimination (or retro‐hydroboration) versus R? H elimination, depending on the R group on the B atom and the chelate backbone. Mechanistic aspects of these highly unusual reactions have been established from both experimental and computational evidence. Adduct formation between HBR₂ and A was found to be the key intermediate in 1,1‐hydroboration of A .     

The Nature of Aqueous Solutions: Insights into Multiple Facets of Chemistry and Biochemistry from Freezing‐Point Depressions

Contrary to current widely held beliefs, many concentrated aqueous solutions of electrolytes and nonelectrolytes behave ideally. For both, the same simple equation yields mole fractions of water that are equal to the theoretical activities of water. No empirical activity coefficients or ad hoc parameters are needed. Thermodynamic hydration numbers and the number of particles produced per mole of solute are found by searching freezing‐point depression measurements, as if asking the water, “How much available water solvent is left and how many solute particles are there?” The results answer questions currently under debate: Do solutes alter the nature of water outside their immediate surroundings? What is the number of ion pairs formed by various electrolytes and what affects extents of their formation? What are some factors that cause precipitation of proteins, latexes, and so forth from aqueous solutions upon addition of other solutes (Hofmeister series)? Which nonelectrolytes form aggregates in water and what are the implications? Why do different solutes affect viscosity differently? How do ion‐selective channels in cell membranes function at the molecular level?