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2
Pixelwise high-temperature calibration for in-situ temperature measuring in powder bed fusion of metal with laser beam.用于金属粉末床激光束熔合原位温度测量的逐像素高温校准
Heliyon. 2024 Apr 2;10(7):e28989. doi: 10.1016/j.heliyon.2024.e28989. eCollection 2024 Apr 15.
3
Thermometries for Single Nanoparticles Heated with Light.用光加热的单个纳米粒子的测温法。
ACS Sens. 2024 Mar 22;9(3):1049-1064. doi: 10.1021/acssensors.4c00012. Epub 2024 Mar 14.
4
Crystallinity swayed phase transformation and oxygen vacancy formation in TiO aerogel photocatalysts.TiO 气凝胶光催化剂中的结晶度对相转变和氧空位形成的影响。
Environ Res. 2023 Dec 15;239(Pt 2):117409. doi: 10.1016/j.envres.2023.117409. Epub 2023 Oct 12.
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Pulsed Photothermal Heterogeneous Catalysis.脉冲光热多相催化
ACS Catal. 2023 Feb 22;13(5):3419-3432. doi: 10.1021/acscatal.2c05435. eCollection 2023 Mar 3.
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Phase transition of individual anatase TiO microcrystals with large percentage of (001) facets: a Raman mapping and SEM study.具有大比例(001)晶面的锐钛矿 TiO 微晶体的相转变:拉曼映射和 SEM 研究。
Phys Chem Chem Phys. 2023 Jan 27;25(4):3199-3210. doi: 10.1039/d2cp04882e.
7
The Anatase-to-Rutile Phase Transition in Highly Oriented Nanoparticles Array of Titania with Photocatalytic Response Changes.具有光催化响应变化的二氧化钛高度取向纳米颗粒阵列中的锐钛矿相到金红石相的转变
Nanomaterials (Basel). 2022 Dec 11;12(24):4418. doi: 10.3390/nano12244418.
8
Optical Hydrogen Nanothermometry of Plasmonic Nanoparticles under Illumination.光激发等离子体纳米粒子的光学氢纳米测温法。
ACS Nano. 2022 Apr 26;16(4):6233-6243. doi: 10.1021/acsnano.2c00035. Epub 2022 Mar 28.
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热等离子体加热能达到何种程度:金纳米颗粒等离子体加热导致的P25 TiO₂的相变与熔化

How Hot Plasmonic Heating Can Be: Phase Transition and Melting of P25 TiO from Plasmonic Heating of Au Nanoparticles.

作者信息

Lu Weigang, Kayastha Rohil, Birmingham Blake, Zechmann Bernd, Zhang Zhenrong

机构信息

Department of Physics, Baylor University, Waco, Texas 76798, United States.

Center for Microscopy and Imaging, Baylor University, Waco, Texas 76798, United States.

出版信息

ACS Appl Mater Interfaces. 2025 Jun 4;17(22):33047-33058. doi: 10.1021/acsami.5c03004. Epub 2025 May 19.

DOI:10.1021/acsami.5c03004
PMID:40388690
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12147774/
Abstract

Plasmonic heating has been utilized in many applications, including photocatalysis, photothermal therapy, and photocuring. However, the heat dissipation process of plasmonic nanoparticles (NPs) and the surrounding matrix is complex. How high the temperature of the matrix that surrounds the plasmonic NPs, such as the catalyst and substrate, can reach is unclear. Herein, we study the dissipation of plasmonic heat generated by resonantly excited gold (Au) NPs dispersed on a P25 TiO NP porous film in air. Under resonant 532 nm continuous wave (CW) laser irradiation at the surface of Au-TiO, the surface evaporation and the aggregation of Au NPs were observed at moderate laser power. This process is accompanied by the phase transition of TiO. More importantly, the TiO NP film melted, forming melt pools and a molten TiO matrix. This indicates that the temperature of TiO reached as high as its melting point of 1830 °C. When Au/TiO was irradiated with an off-resonance laser at 638 nm, no phase transformation or melting of TiO was observed. The temperature calculation showed that the heating generated by Au NPs is not localized. The collective heating from an ensemble of Au NPs in the irradiated area produced a global temperature increase that melted TiO. Our results suggest that the photothermal effect could be a significant mechanism in the plasmon-assisted photocatalytic reactions.

摘要

等离子体加热已被应用于许多领域,包括光催化、光热疗法和光固化。然而,等离子体纳米颗粒(NPs)与周围基质的散热过程很复杂。尚不清楚围绕等离子体NPs的基质(如催化剂和底物)能达到多高的温度。在此,我们研究了分散在空气氛围中的P25 TiO NP多孔膜上的共振激发金(Au)NPs产生的等离子体热的耗散情况。在Au-TiO表面用532 nm连续波(CW)激光进行共振照射时,在中等激光功率下观察到了Au NPs的表面蒸发和聚集现象。此过程伴随着TiO的相变。更重要的是,TiO NP膜熔化,形成熔池和熔融的TiO基质。这表明TiO的温度高达其熔点1830℃。当用638 nm的非共振激光照射Au/TiO时,未观察到TiO的相变或熔化现象。温度计算表明,Au NPs产生的加热并非局限于局部。照射区域内Au NPs集合体的集体加热导致了整体温度升高,从而使TiO熔化。我们的结果表明,光热效应可能是等离子体辅助光催化反应中的一个重要机制。