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Resonant secondary light emission from plasmonic Au nanostructures at high electron temperatures created by pulsed-laser excitation

机译:脉冲激光激发在高电子温度下从等离子体Au纳米结构产生的共振二次光发射

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摘要

Plasmonic nanostructures are of great current interest as chemical sensors, in vivo imaging agents, and for photothermal therapeutics. We study continuous-wave (cw) and pulsed-laser excitation of aqueous suspensions of Au nanorods as a model system for secondary light emission from plasmonic nanostructures. Resonant secondary emission contributes significantly to the background commonly observed in surface-enhanced Raman scattering and to the light emission generated by pulsed-laser excitation of metallic nanostructures that is often attributed to two-photon luminescence. Spectra collected using cw laser excitation at 488 nm show an enhancement of the broad spectrum of emission at the electromagnetic plasmon resonance of the nanorods. The intensity of anti-Stokes emission collected using cw laser excitation at 785 nm is described by a 300 K thermal distribution of excitations. Excitation by subpicosecond laser pulses at 785 nm broadens and increases the intensity of the anti-Stokes emission in a manner that is consistent with electronic Raman scattering by a high-temperature distribution of electronic excitations predicted by a two-temperature model. Broadening of the pulse duration using an etalon reduces the intensity of anti-Stokes emission in quantitative agreement with the model. Experiments using a pair of subpicosecond optical pulses separated by a variable delay show that the timescale of resonant secondary emission is comparable to the timescale for equilibration of electrons and phonons.
机译:等离子体等离子纳米结构作为化学传感器,体内成像剂以及光热疗法在当前引起了极大的兴趣。我们研究金纳米棒的水悬浮液的连续波(cw)和脉冲激光激发作为等离子体系统纳米结构二次发光的模型系统。共振二次发射极大地促进了通常在表面增强拉曼散射中观察到的本底,以及通常由双光子发光引起的金属纳米结构的脉冲激光激发所产生的光发射。使用连续波激光在488 nm激发下收集的光谱显示出纳米棒的电磁等离子体共振时发射光谱的增强。使用300 K激发热分布来描述使用785 nm连续激光激发收集的反斯托克斯发射强度。亚皮秒激光脉冲在785 nm处的激发以与电子拉曼散射一致的方式加宽并增加了反斯托克斯发射的强度,该方式与通过两个温度模型预测的电子激发的高温分布一致。使用标准具加宽脉冲持续时间可降低反斯托克斯发射的强度,从而与模型定量吻合。使用一对由可变延迟分开的亚皮秒光脉冲进行的实验表明,共振二次发射的时间尺度与电子和声子平衡的时间尺度相当。

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