Photoreduction on a periodically proton exchanged ferroelectric crystal leads to the formation of periodic metallic nanostructures on the surface. By varying the depth of the proton exchange (PE) from 0.59 to 3.10 μm in congruent lithium niobate crystals, the width of the lateral diffusion region formed by protons diffusing under the mask layer can be controlled. The resulting deposition occurs in the PE region with the shallowest PE depth and preferentially in the lateral diffusion region for greater PE depths. PE depth-control provides a route for the fabrication of complex metallic nanostructures with controlled dimensions on chemically patterned ferroelectric templates.

Local reactivity on periodically proton exchanged lithium niobate (PPE:LN) surfaces is a promising route for the fabrication of regularly spaced nanostructures. Here, using MgO-doped PPE:LN templates, we investigate the influence of the doping on the nanostructure formation as a function of the proton exchange (PE) depth. The deposition is found to occur preferentially along the boundary between MgO-doped LN and the PE region when the PE depth is at least 1.73 μm, however, for shallower depths, deposition occurs across the entire PE region. The results are found to be consistent with an increased photoconductivity of the MgO-doped LN.

Cystic Fibrosis (CF) and Duchenne Muscular Dystrophy (DMD) are well characterized progressive inherited diseases associated with significant morbidity and mortality. Therefore, the early, rapid and affordable diagnosis of these disorders through newborn screening is highly important for the appropriate management. Here, we report label‐free impedance immunosensors for the simple screening of CF and DMD through the detection of cystic fibrosis transmembrane conductance regulator (CFTR) protein fragment and a peptide sequence for dystrophin (DMD). The biosensors were constructed by the covalent immobilization of specific antibodies for CFTR and DMD on standard gold (Au) electrodes. The immunosensors response was measured based on the change in the electrochemical impedance spectroscopy (EIS) signals after binding with the peptides. The specific recognition of the immunosensor surfaces to the target antigens leads to retardation of the access of ferri‐ferrocyanide redox molecules to the surface and thus, enhances the charge transfer resistance (Rct). These impedimetric immunosensors enabled sensitive, fast, selective and accurate estimation of CFTR and DMD levels within a linear range from 1.0 pg/mL to 1 μg/mL and 1.0 pg/mL to 10 ng/mL with lower detection limits of 0.8 and 0.7 pg/mL for CFTR and DMD, respectively. Moreover, the immunosensors were tested for the detection of CFTR and DMD in human serum showing very good agreement with enzyme‐linked immunosorbent assays (ELISA). This work represents a novel low cost analytical method that aims to satisfy the unmet public health need in the early diagnosis of CF and DMD and can be extended to detect other hereditary disorders.

Oxide phase nanowires are important for applications ranging from optoelectronics to water splitting, but prove difficult to grow in high density with good crystalline quality and phase purity. Heterogeneous catalysts are typically required to nucleate growth. This work demonstrates that dispersions of oxide nanowires can be formed directly from solution processed oxide thin films. We also examine the effect of changes in applied pressure between a solution processed vanadium oxide thin film and a surface-contacted glass coupon on the catalyst-free formation of interconnected sodium vanadate nanowire structures by interdiffusion. Under different applied pressures, meshes of high quality crystalline oxide nanowires formed on the surface, and we examine the nature of phase conversion and nanostructure growth including larger shards composed of multiple conjoined nanowires are also examined. The optical properties of the oxides NWs formed by interdiffusion from oxide thin films show promising properties for application as antireflective coatings across a broadband spectral range. This interdiffusion technique is effective for high quality oxide nanowire growth without catalysts directly from insulating or conducting thin films by direct contact with a source of diffusing species. The integration of nanowires (NWs) with modern devices and systems is advancing considerably each year with new applications, from electronics/optoelectronics to energy storage/generation, availing of these nanosized structures as active materials.1-4 NWs can be made from a variety of materials each with their own specific applications, from metal to semiconducting NWs for use in applications such as transparent conducting electrodes, anti-reflection (AR) coatings, sensors, solar cells and photonics.2,5-9 Improved methods for the incorporation of NWs with other device components, such as ensuring intimate electrical/thermal contact with the underlying substrate, requires better control and understanding of the NW growth processes. Investigation of improvements into the deposition methods for NWs also needs to focus on improved control over the growth, optical/electrical properties and site selectivity using a variety of techniques through both top-down and bottom-up processes. [10][11][12][13] Applications such as transistor technologies require that there are no erroneous signals or crosstalk between each device; in situations such as this the growth and deposition technique of the NWs requires intricate and exacting methods to accomplish high site selectivity onto the substrates.14,15 However, this site selective single NW deposition is not required for every application; instead large interconnected NW networks with random orientations are more desirable and also easier to deposit. Interconnected NW networks are used for catalysis, photonics and sensing applications where the random orientations, high surface areas and increased electrical connections improves the light absorption/scattering, sensor sensitivity and the electrical conduc...