7 research outputs found

    Registration-Free Hybrid Learning Empowers Simple Multimodal Imaging System for High-quality Fusion Detection

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    Multimodal fusion detection always places high demands on the imaging system and image pre-processing, while either a high-quality pre-registration system or image registration processing is costly. Unfortunately, the existing fusion methods are designed for registered source images, and the fusion of inhomogeneous features, which denotes a pair of features at the same spatial location that expresses different semantic information, cannot achieve satisfactory performance via these methods. As a result, we propose IA-VFDnet, a CNN-Transformer hybrid learning framework with a unified high-quality multimodal feature matching module (AKM) and a fusion module (WDAF), in which AKM and DWDAF work in synergy to perform high-quality infrared-aware visible fusion detection, which can be applied to smoke and wildfire detection. Furthermore, experiments on the M3FD dataset validate the superiority of the proposed method, with IA-VFDnet achieving the best detection performance than other state-of-the-art methods under conventional registered conditions. In addition, the first unregistered multimodal smoke and wildfire detection benchmark is openly available in this letter

    Phase transition and electron localization in 1TTaS2\mathrm{1T-TaS_2}

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    The magnetic properties and phase transitions of 1T-TaS2_2 and 1T-Fe0.07_{0.07}Ta0.93_{0.93}S2_2 have been studied in the interval of 1.5–300 K and over the range of 100 Oe–60 kOe. Experimental results show that at high temperatures the compounds are in a diamagnetic state and the commensurate-charge-density-wave–triclinic-nearly-commensurate transition temperature of 1T-TaS2_2 decreases with increasing magnetic field. The amount of variation is a function of the magnetic field. At low temperatures both 1T-TaS2_2 and 1T-Fe0.07_{0.07}Ta0.93_{0.93}S2_{2} are in a paramagnetic state owing to the localized moments that come from the single Anderson-Mott localization state. The curves of magnetization versus temperature do not follow the Curie law or Curie-Weiss law, but can be described fairly well as M=M0_0+T\sqrt T−n. The fitting parameters of experimental curves show that a part of the neighboring moment appears as antiferromagnetic coupling due to exchange interaction between the moments. The magnetic-field dependence of magnetization exhibits a complicated feature at low temperature. It shows that the compounds may undergo a phase transition at the maximum value of magnetization and then they are probably in a mixed charge-density-wave–spin-density-wave (CDW-SDW) state or SDW state due to the coherent superposition of the antiferromagnetic coupling

    Tuning Electrochemical Properties of Li-Rich Layered Oxide Cathodes by Adjusting Co/Ni Ratios and Mechanism Investigation Using in situ X‑ray Diffraction and Online Continuous Flow Differential Electrochemical Mass Spectrometry

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    Owing to high specific capacity of ∼250 mA h g<sup>–1</sup>, lithium-rich layered oxide cathode materials (Li<sub>1+<i>x</i></sub>Ni<sub><i>y</i></sub>Co<sub><i>z</i></sub>Mn<sub>(3–<i>x</i>–2<i>y</i>–3<i>z</i>)/4</sub>O<sub>2</sub>) have been considered as one of the most promising candidates for the next-generation cathode materials of lithium ion batteries. However, the commercialization of this kind of cathode materials seriously restricted by voltage decay upon cycling though Li-rich materials with high cobalt content have been widely studied and show good capacity. This research successfully suppresses voltage decay upon cycling while maintaining high specific capacity with low Co/Ni ratio in Li-rich cathode materials. Online continuous flow differential electrochemical mass spectrometry (OEMS) and in situ X-ray diffraction (XRD) techniques have been applied to investigate the structure transformation of Li-rich layered oxide materials during charge–discharge process. The results of OEMS revealed that low Co/Ni ratio lithium-rich layered oxide cathode materials released no lattice oxygen at the first charge process, which will lead to the suppression of the voltage decay upon cycling. The in situ XRD results displayed the structure transition of lithium-rich layered oxide cathode materials during the charge–discharge process. The Li<sub>1.13</sub>Ni<sub>0.275</sub>Mn<sub>0.580</sub>O<sub>2</sub> cathode material exhibited a high initial medium discharge voltage of 3.710 and a 3.586 V medium discharge voltage with the lower voltage decay of 0.124 V after 100 cycles
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