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Methane (CH), as the main component of natural gas and coal mine gas, is widely used in daily life and industrial processes and its leakage always causes undesirable misadventures. Thus, the rapid detection of low concentration methane is quite necessary. However, due to its robust chemical stability resulting from the strong tetrahedral-symmetry structure, the methane molecules are usually chemically inert to the sensing layers in detectors, making the rapid and efficient alert a big challenge. In this work, palladium nanoparticles (Pd NPs) embedded indium oxide porous hollow tubes (InO PHTs) were successfully synthesized using Pd@MIL-68 (In) MOFs as precursors. All InO-based samples derived from Pd@MIL-68 (In) MOFs inherited the morphology of the precursors and exhibited the feature of hexagonal hollow tubes with porous architecture. The gas-sensing performances to 5000 ppm CH were evaluated and it was found that Pd@InO-2 gave the best response (R/R = 23.2) at 370 °C, which was 15.5 times higher than that of pristine-InO sensors. In addition, the sensing materials also showed superior selectivity against interfering gases and a rather short response/recovery time of 7 s/5 s. The enhancement in sensing performances of Pd@InO-2 could be attributed to the large surface area, rich porosity, abundant oxygen vacancies and the catalytic function of Pd NPs.
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http://dx.doi.org/10.3390/s23031163 | DOI Listing |
Int J Biol Macromol
September 2025
Department of Biomedical Engineering, IIT Hyderabad, Kandi, Sangareddy, Telangana 502285, India. Electronic address:
While 3D bioprinting has advanced tissue engineering, the creation of complex, self-supporting structures like hollow tubes has complexities that catalyzed the emergence of 4D bioprinting. Our study introduces a novel approach inspired by nature's ability to create dynamic, hollow structures-such as curling leaves that adapt to environmental conditions through moisture absorption and deswelling. We present a cutting-edge 4D bioprinting method that enables the precise, controlled formation of hollow tubes with varying sizes, utilizing functionally modified silk (namely SilMA) (10-20 %) and its composites (prepared with 0.
View Article and Find Full Text PDFACS Electrochem
August 2025
Technical University of Munich (TUM), Campus Straubing for Biotechnology and Sustainability, Uferstraße 53, 94315 Straubing, Germany.
The pore structure is a key design parameter for optimizing electrocatalytic systems that utilize porous electrodes, necessitating characterization at scales relevant to catalysis (∼0.1-100 μm). In this Review, we examine how diffusion during faradaic processes is impacted by the electrode pore geometry, defined by the concavity/convexity of its surface curvature, and by pore size, defined by the finiteness of the diffusion domain.
View Article and Find Full Text PDFA novel ultra-wideband low-loss miniaturized 3 dB coupler based on a polymer dual-hollow-core anti-resonant fiber (DHC-ARF) is proposed. The wavelength dependence can be effectively reduced by adopting two identical elliptical cores in the DHC-ARF and the polarization dependence can be greatly weakened by introducing two small nested tubes into two cladding tubes at both sides of the air-gap channel between two cores. The 3 dB coupler can be constructed by a 4.
View Article and Find Full Text PDFOpt Express
February 2025
A single-polarization hollow-core anti-resonant fiber (HC-ARF) with nested stadium-shaped tubes is proposed for single mode, low loss, and high birefringence characteristics. X-pol fundamental mode (FM) is coupled to the cladding mode (CM) by introducing four anti-resonant tubes and one resonant tube. Y-pol FM is tightly bound in the fiber core, thus achieving a high polarization extinction ratio (PER).
View Article and Find Full Text PDFWe report a simple and effective approach to reversely tailoring the tubes of an antiresonant hollow-core fiber (AR-HCF). The AR-HCFs with elliptical-shaped shrinkage tubes, implemented by a traditional flame brushing technique, were characterized for what we believe to be the first time. We have thus achieved a 70 nm wide bandpass filter with a minimum extra loss below 0.
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