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金纳米棒/铜硫属化合物核壳纳米结构中表面等离子体的耦合共振及其增强的光热效应

Coupling Resonances of Surface Plasmon in Gold Nanorod/Copper Chalcogenide Core-Shell Nanostructures and Their Enhanced Photothermal Effect.

作者信息

Li Yingying, Pan Guiming, Liu Qiyu, Ma Liang, Xie Ying, Zhou Li, Hao Zhonghua, Wang Ququan

机构信息

Department School of Physics and Technology, Wuhan University, Wuhan, 430072, P. R. China.

School of Science, Wuhan Institute of Technology, Wuhan, 430072, P. R. China.

出版信息

Chemphyschem. 2018 Jun 4. doi: 10.1002/cphc.201701338.

Abstract

Dual plasmonic Au@Cu S core-shell nanorods (NRs) have been fabricated by using a hydrothermal method and plasmon-coupled effect between the Au core and Cu S shell in the near-infrared (NIR) region. The extinction spectrum of Au@Cu S NRs is dominated by the surface plasmon resonance (SPR) of the Cu S shell, the transverse surface plasmon resonance (TSPR), and the longitudinal surface plasmon resonance (LSPR) of the Au NRs. With the Cu S shell increasing (fixed Au NRs), the TSPR peak slightly redshifts and the LSPR and SPR peaks blueshift, owing to competition between the redshift of the refractive index effect and blueshift from the plasmon coupled effect. Although, for Au@Cu S NRs, only TSPR and LSPR peaks can be seen and a redshift arises with the increasing Cu S shell thickness, implying that no plasmonic coupling between Au NRs and Cu S shell occurred. The extinction spectrum of the Au@Cu S NRs with three coupled resonance peaks is simulated by using the FDTD method, taking into account the electron-transfer effect. The dispersion properties of the coupling of Au@Cu S NRs with the LSPR of the initial Au core are studied experimentally by changing the length of the Au NRs, which are explained theoretically by the coupled harmonic oscillator model. The calculated coupled coefficients between SPR of the Cu S shell and LSPR of the Au NRs is 180 meV, which is much stronger than that of TSPR of Au NRs of 55 meV. Finally, the enhanced photothermal effect of Au@Cu S NRs has been demonstrated.

摘要

通过水热法以及金核与硫化铜壳层在近红外(NIR)区域的等离子体耦合效应,制备了双等离子体金@硫化铜核壳纳米棒(NRs)。金@硫化铜纳米棒的消光光谱主要由硫化铜壳层的表面等离子体共振(SPR)、横向表面等离子体共振(TSPR)以及金纳米棒的纵向表面等离子体共振(LSPR)主导。随着硫化铜壳层增加(金纳米棒固定),由于折射率效应的红移与等离子体耦合效应的蓝移之间的竞争,TSPR峰略微红移,而LSPR和SPR峰蓝移。尽管对于金@硫化铜纳米棒,只能看到TSPR和LSPR峰,并且随着硫化铜壳层厚度增加会出现红移,这意味着金纳米棒与硫化铜壳层之间没有发生等离子体耦合。考虑到电子转移效应,使用时域有限差分(FDTD)方法模拟了具有三个耦合共振峰的金@硫化铜纳米棒的消光光谱。通过改变金纳米棒的长度,实验研究了金@硫化铜纳米棒与初始金核的LSPR耦合的色散特性,并通过耦合谐振子模型进行了理论解释。计算得到的硫化铜壳层SPR与金纳米棒LSPR之间的耦合系数为180毫电子伏特,这比金纳米棒TSPR的55毫电子伏特要强得多。最后,证明了金@硫化铜纳米棒增强的光热效应。

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