Ion-induced transient potential fluctuations facilitate pore formation and cation transport through lipid membranes

Unassisted ion transport through lipid membranes plays a crucial role in many cell functions without which life would not be possible, yet the precise mechanism behind the process remains unknown due to its molecular complexity. Here, we demonstrate a direct link between membrane potential fluctuations and divalent ion transport. High-throughput wide-field second harmonic (SH) microscopy shows that membrane potential fluctuations are universally found in lipid bilayer systems. Molecular dynamics simulations reveal that such variations in membrane potential reduce the free energy cost of transient pore formation and increase the ion flux across an open pore. These transient pores can act as conduits for ion transport, which we SH image for a series of divalent cations (Cu$^{2+}$, Ca$^{2+}$, Ba$^{2+}$, Mg$^{2+}$) passing through GUV membranes. Combining the experimental and computational results, we show that permeation through pores formed via an ion-induced electrostatic field is a viable mechanism for unassisted ion transport.Comment: 8 pages, 2 figure

Passive and active ion permeation through lipid bilayers investigated by second harmonic water imaging

Lipid membranes are complex and dynamic systems which are known to mediate signaling processes between cells and their environment. To do this multiple ion channels and pumps are involved in controlling the in- and out-flux of various ions (K+, Na+, Mg2+, Ca2+, etc.) and help maintain and regulate a concentration gradient of ions across the membrane. Additionally, membranes are semi-permeable for some species including water and even ions. However, molecular level information about passive and active transport of ions across lipid membranes is either missing or incomplete and ignores membrane hydration without which a membrane would not self-assemble. In this project, we use high-throughput wide-field second harmonic (SH) microscopy to learn about the molecular level structure of membrane interfaces during those processes by imaging the non-resonant response of interfacial water. We show that this technique is extremely sensitive to the transmembrane distribution of interfacial ions which disturb membrane hydration and thus change SH contrast. We apply this technique to probe the molecular structure(orientational order of water, strength of ion binding) at the interfaces of freestanding lipid bilayers and giant unilamellar vesicles (GUVs). We start with SH imaging of operational voltage-gated alamethicin ion channels in freestanding lipid membranes surrounded by an aqueous solution on either side. We observe a change in SH intensity upon channel activation that is traced back to a change in the orientational distribution of water molecules caused by transported ions. Of the transported ions, a fraction of 10-4 arrives at the hydrated membrane interface, leading to interfacial electrostatic changes on the time scale of a second. Later on, in order to improve SH contrast from low-emitting samples (such as interfacial water) and thus be able to study even more fundamental and delicate surface processes, we develop and build a femtosecond optical parametric amplifier. This laser system generates a tunable output in the range from 670 nm to 1000 nm at a 1 MHz repetition rate with a minimum pulse duration of 23 fs at 900 nm. Comparing our current femtosecond laser system with the new one at equal fluences we experimentally observe a 30 times improvement in SH contrast of low-emitting samples. Then, we present a new approach of label-free second harmonic imaging of GUV hydration which directly reports on the cross-membrane distribution of divalent cations bound to negatively charged lipid headgroups. We use this property to study passive transport of Ca2+ ions through lipid membranes. By varying the hydrophobic core of the bilayer, we observe Ca2+ translocation for mono-unsaturated (DOPC:DOPA) membranes which is reduced upon adding cholesterol. A complete inhibition of translocation is observed for branched (DPhPC:DPhPA) and poly-unsaturated (SLPC:SLPA) lipid membranes. In order to gain more insight into the mechanism of divalent cation transport, we perform a series of experiments with different ions (Mg2+, Ba2+, Ca2+and Cu2+). Surprisingly, we observe translocation of Ba2+, Ca2+ and Cu2+ ions through unsaturated DOPC:DOPA membranes which fully neutralize the inner membrane leaflet. Translocation time increases in the order Cu2+< Ca2+< Ba2+, while Mg2+ ions do not show any permeation. The observed trend in passive transport correlates with a trend in ion binding strength measured on impermeable GUVs with the same headgroup composition.LB

Continuous compensation of the phase mismatch by using temperature gradients for second harmonic generation

The second harmonic of an infrared laser generated by frequency doubling in a nonlinear crystal can be adversely affected by group delay dispersion applied to the fundamental radiation. Yet large amounts of group delay dispersion can be advantageous when using periodically poled crystals with a linearly chirped period. We propose to achieve the same effects with continuous variation of the phase mismatch in the propagation direction, by applying a temperature gradient to a lithium triborate crystal. Advantageously the temperature gradient can be adjusted depending on the desired results. We demonstrate, through both simulation and experiment, an improvement in not only second harmonic conversion efficiency and beam quality, but also that the second harmonic duration and is bandwidth can be controlled with the temperature gradient

Interaction of Oil and Lipids in Freestanding Lipid Bilayer Membranes Studied with Label-Free High-Throughput Wide-Field Second-Harmonic Microscopy

The interaction of oils and lipids is relevant for membrane biochemistry since the cell uses bilayer membranes, lipid droplets, and oily substances in its metabolic cycle. In addition, a variety of model lipid membrane systems, such as freestanding horizontal membranes and droplet interface bilayers, are made using oil to facilitate membrane monolayer apposition. We characterize the behavior of excess oil inside horizontal freestanding lipid bilayers using different oils, focusing on hexadecane and squalene. Using a combination of second-harmonic (SH) and white-light imaging, we measure how oil redistributes within the membrane bilayer after formation. SH imaging shows that squalene forms a wider annulus compared with hexadecane, suggesting that there is a higher quantity of squalene remaining in the bilayer compared with hexadecane. Excess oil droplets that appear right after membrane formation are tracked with white-light microscopy. Hexadecane droplets move directionally to the edge of the membrane with diffusion constants similar to those of single lipids, whereas squalene oil droplets move randomly with lower diffusion speeds similar to lipid condensed domains and remain trapped in the center of the bilayer for ∼1–3 h. We discuss the observed differences in terms of different coupling mechanisms between the oil and lipid molecules induced by the different chemical structures of the oils

Spatiotemporal Imaging of Water in Operating Voltage-Gated Ion Channels Reveals the Slow Motion of Interfacial Ions

Ion channels are responsible for numerous physiological functions ranging from transport to chemical and electrical signaling. Although static ion channel structure has been studied following a structural biology approach, spatiotemporal investigation of the dynamic molecular mechanisms of operational ion channels has not been achieved experimentally. In particular, the role of water remains elusive. Here, we perform label-free spatiotemporal second harmonic (SH) imaging and capacitance measurements of operational voltage-gated alamethicin ion channels in freestanding lipid membranes surrounded by aqueous solution on either side. We observe changes in SH intensity upon channel activation that are traced back to changes in the orientational distribution of water molecules that reorient along the field lines of transported ions. Of the transported ions, a fraction of 10–4 arrives at the hydrated membrane interface, leading to interfacial electrostatic changes on the time scale of a second. The time scale of these interfacial changes is influenced by the density of ion channels and is subject to a crowding mechanism. Ion transport along cell membranes is often associated with the propagation of electrical signals in neurons. As our study shows that this process is taking place over seconds, a more complex mechanism is likely responsible for the propagation of neuronal electrical signals than just the millisecond movement of ions

Narrowband photoluminescence of Tin-Vacancy colour centres in Sn-doped chemical vapour deposition diamond microcrystals

Tin-Vacancy (Sn-V) colour centres in diamond have a spin coherence time in the millisecond range at temperatures of 2 K, so they are promising to be used in diamond-based quantum optical devices. However, the incorporation of large Sn atoms into a dense diamond lattice is a non-trivial problem. The objective of our work is to use microwave plasma-assisted chemical vapour deposition (CVD) to grow Sn-doped diamond with submicron SnO2 particles as a solid-state source of impurity. Well-faceted diamond microcrystals with sizes of a few micrometres were formed on AlN substrates. The photoluminescence (PL) signal with zero-phonon line (ZPL) peak for Sn-V centre at ≈620 nm was measured at room temperature (RT) and at 7 K. The peak width (full width at half-maximum) was measured to be 1.1–1.7 nm at RT and ≈0.05 nm at 7 K. The observed variations of ZPL shape and position, in particular, narrowing of PL peak at RT and formation of single-line fine structure at low-T, are attributed to strain in the crystallites. The diamond doping with Sn via CVD process offers a new route to from Sn-V colour centre in the bulk of the diamond crystallites

Investigation of materials for supercontinuum generation for subsequent nonlinear parametrical and Raman amplification at 1 MHz repetition rate

In the present work we performed research of supercontinuum generation in several commonly used and new supercontinuum generation crystals for subsequent nonlinear amplification, using 1-3 mu J energy pulses of 300 fs duration at 1 MHz repetition rate. Obtained supercontinuum spectra spanning over 480-1950 nm wavelength range at pump pulse energies as low as 200nJ in KGW and YVO4 crystals. We present simple experimental setups of stimulated Raman amplification and optical parametric amplification using supercontinuum seeds obtained from several selected crystals. We achieved total energy conversion efficiencies up to 9% both for optical parametric amplification setup and for stimulated Raman amplification setups. The optical parametric amplifier was tunable in the 680-980 nm spectral range and produced ultrashort pulses of 23-44 fs duration. Raman amplifier produced more than 130 mW average power at 1194 nm wavelength and featured broadened spectrum corresponding to Fourier transform limited similar to 100 fs pulse duration. We demonstrated that low power and low energy femtosecond lasers could be efficiently employed for the nonlinear wavelength conversion