Tunable laser | EPFL Graph Search

A tunable laser is a laser whose wavelength of operation can be altered in a controlled manner. While all laser gain media allow small shifts in output wavelength, only a few types of lasers allow continuous tuning over a significant wavelength range. There are many types and categories of tunable lasers. They exist in the gas, liquid, and solid state. Among the types of tunable lasers are excimer lasers, gas lasers (such as CO2 and He-Ne lasers), dye lasers (liquid and solid state), transition metal solid-state lasers, semiconductor crystal and diode lasers, and free electron lasers. Tunable lasers find applications in spectroscopy, photochemistry, atomic vapor laser isotope separation, and optical communications. Types of tunability Single line tuning Since no real laser is truly monochromatic, all lasers can emit light over some range of frequencies, known as the linewidth of the laser transition. In most lasers, this linewidth is quite narrow (for example, th

Micromachined tunable devices based on silicon integrated BaxSr1-xTiO3 thin films

Andreas Nöth

Thin Film Bulk Acoustic Wave Resonators (TFBARs) had been developed a decade ago and since then were implemented extensively in mobile communications devices. The "heart" of a TFBAR consists of a piezoelectric film that operates as an acousto-electric transducer, stabilizing the transmission at a given predetermined frequency. For reasons such as space economy in hand-held devices, it is of interest to make these TFBARs tunable, so that a single TFBAR is multi-band responsive. This thesis demonstrates for the first time electrically tunable, single-component TFBARs. A theory describing the tuning behavior of dc bias induced acoustic resonances was developed. Then we made the hypothesis that dc bias induced piezoelectric BaxSr1-xTiO3 (BST) thin films – namely, paraelectric, non-piezoelectric films operating under dc bias – can be used to make electrically tunable TFBARs and that the devices can be switched on or off depending on the dc bias state. The devices were then fabricated: We integrated BST lms onto silicon substrates, micromachined the substrate to create the TFBARs and a new type of suspended planar capacitor which were then characterized, analyzed, and modeled, demonstrating successfully the new concept: We developed a theory describing the electrical tuning behavior of the dc bias induced acoustic resonances in paraelectric thin lms in terms of material parameters. The field dependent constitutive piezoelectric equations were derived from the Landau free energy P-expansion by taking the linear and nonlinear electrostrictive terms as well as the background permittivity into account. We considered two modes of excitation for the tuning of the acoustic resonances, namely the thickness excitation (TE) mode and the lateral field excitation (LFE) mode. The tuning behavior of the two types of resonators based on BST thin films was modeled and discussed. For the modeling we calculated the relevant tensor components controlling the tuning of the BST resonators from the available literature data. The fabrication of the membrane-type TFBARs was realized by integrating BST thin films onto silicon substrates and using micromaching technologies. We showed that the developed TFBARs can be switched on or off with a dc bias. At a dc electric field of 615 kV/cm we observed a tuning of -2.4% (-66 MHz) and -0.6% (-16 MHz) for the resonance and antiresonance frequencies of the device, while the resonance frequency at a dc electric field extrapolated to 0 kV/cm was 2.85 GHz. The effective electromechanical coupling factor k2eff of the device increased up to 4.4%. The tuning was non-hysteretic. The Quality-factor (Q-factor) of the device was about 200. The developed micromaching processes for the TFBARs were used to fabricate coplanar BST capacitors on silicon. Micromaching was used to remove the Si substrate under the active area of the device. Comparing this new micromachined coplanar capacitor with conventional non-micromachined capacitors, we demonstrated that the removal of the substrate from the active device area resulted in a reduction of parasitic effects. The micromachined coplanar capacitor showed an increased tunability and a reduced loss tangent in comparison to the non-micromachined capacitor. The micromachined capacitor showed a relative tunability of 37% at a dc electric field of 1100 kV/cm. The loss tangent was 0.08 and 0.06 at zero and maximum dc bias, respectively, at a measurement frequency of 20 GHz. The integration of epitaxial BST thin films on silicon was studied as well because of its potential improvement of the device performance in comparison to devices based on polycrystalline films. Two different electrode/buffer layer systems, YBa2Cu3O7-x (YBCO) / CeO2 / YxZr1-xO2-x/2 (YSZ) and TiN were used for the integration. Epitaxial BST thin films were grown with both structures. For the BST / YBCO / CeO2 / YSZ / Si structure, the BST unit cell was rotated by 45° in the in-plane dimension with respect to the substrate. The BST layer exhibited good structural quality as indicated by a Full Width at Half Maximum (FWHM) of 0.5° of the rocking curve of the BST(002) diffraction peak. For the BST / TiN / Si structure, the BST layer was grown with a cube-on-cube epitaxial relationship on the silicon substrate, thus demonstrating epitaxially grown BST on silicon using conventional bottom electrode that is easily acceptable by the microelectronic industry. However, in this case, the structural quality of the BST layer was reduced in comparison to the BST / YBCO / CeO2 / YSZ / Si structure. The FWHM of the rocking curve of the BST(002) diffraction peak was 2.2°. We established the temperature (T=550 to 600 °C) and pressure (p ≈ 10-7 to 5 × 10-4 Torr) conditions for the growth of epitaxial BST thin films on TiN-buffered Si. At too high temperatures and/or oxygen pressures epitaxial BST thin film growth was impeded due to the oxidation of the TiN layer. By introducing experimental results from the electrical characterization of the micromachined devices with the polycrystalline BST into our developed theory, we could successfully model the tuning behavior of our fabricated TFBARs. The modeling allowed us to de-embed the intrinsic electromechanical properties of a freestanding BST layer. The effect of increasing mechanical load on the tuning performance of the device was modeled and studied experimentally. Under strong mechanical load, the tuning of both resonance and antiresonance frequency was reduced. The effect was attributed to a reduction in the tuning of k2eff of the device and of the sound velocity of the BST layer.

EPFL2009

Water as a contrast agent for imaging interfacial structure and ion transport in giant vesicles

David Roesel

Hydrated lipid bilayer membranes and their asymmetry play a fundamental role in living cells by maintaining and regulating concentration gradients between cells, their environment, and their compartments. They achieve this not only through various channels and transporters, but also by being inherently semi-permeable to various molecules, including water and ions. However, molecular information about passive ion transport, as well as the complex structure of membrane hydration remain elusive, mainly due to a lack of experimental methods that can access this information, and relate it to micro- and macroscopic membrane properties. In this work, we study the molecular structure of lipid bilayer membranes and ion transport across them with high throughput wide-field second harmonic (SH) microscopy by utilizing water as the contrast agent. We show that by detecting small amounts of asymmetry in the structure of interfacial water, it is possible to measure the distribution of charged species across the membrane with high sensitivity. We apply this surface-selective technique to measure ion-lipid-water interactions, track ion transport, and quantify electro-chemical surface properties at the interfaces of lipid bilayer membranes in the form of giant unilamellar vesicles (GUVs). We start by improving the throughput of wide field SH microscopy in order to probe low-asymmetry interfaces with high contrast in a label-free manner. To do this, we design a custom optical parametric amplifier (OPA) with a tunable output in the 670-1000 nm range, up to a 1 MHz repetition rate, and an ultra-short 23 fs pulse duration. We then experimentally demonstrate the achieved throughput improvement. Next, we establish a way to probe interfacial hydration of GUVs. We quantify the surface properties of vesicles composed of different ratios of zwitterionic and anionic lipids, and show that only a few percent of anionic headgroups are ionized. We also observe spatial and temporal fluctuations in surface properties, and demonstrate that these fluctuations are universally found in lipid bilayer systems.Following that, we demonstrate a direct link between membrane potential fluctuations and divalent ion transport. Molecular dynamics simulations reveal that these fluctuations 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 (Cu2+, Ca2+, Ba2+, Mg2+) 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.Then, we focus on unassisted Ca2+ translocation in more detail. We vary the hydrophobic core of bilayer membranes and observe different types of behavior in high throughput wide-field SH images. Ca2+ translocation is observed through mono-unsaturated membranes, significantly reduced upon adding cholesterol, and completely inhibited for branched and poly-unsaturated membranes. We propose, using molecular dynamics simulations, that ion transport occurs through ion induced transient pores, which require non-equilibrium membrane restructuring. This results in different transport rates at different locations and suggests that the hydrophobic structure of lipids plays a much more sophisticated regulating role than previously thought.

EPFL2022

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

Maksim Eremchev

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.

EPFL2021