从AU纳米棒,纳米三角形和纳米恒星的表面增强的拉曼散射与调整的等离子体共振
Boris N Khlebtsov1, Andrey M Burov1, Sergey V Zarkov1
1Institute of Biochemistry and Physiology of Plants and Microorganisms, Saratov Scientific Centre of the Russian Academy of Sciences, 13 Prospekt Entuziastov, Saratov 410049, Russia. Khlebtsov@ibppm.ru.
Physical chemistry chemical physics : PCCP
|November 13, 2023
概括
黄金纳米结构的实验数据表明,表面增强拉曼散射 (SERS) 的最佳局部化等离子体共振 (LPR) 与理论不同. LPR波长调整和激发激光器的选择显著影响SERS增强因素.
科学领域:
- 塑学和纳米光子学
- 表面增强的拉曼光谱学 (SERS)
- 纳米材料科学 科学 纳米材料科学
背景情况:
- 电磁理论表明,对于最大的表面增强拉曼散射 (SERS) 增强因子 (EF),最优的局部等离子共振 (LPR) 波长是最佳的,但实验结果往往不同.
- 理论模型预测小拉曼转移的SERS EF尺度与本地场的第四次数,但这种关系并未始终被观察到.
- 选择最佳的等离子共振来最大化SERS信号仍然是一个开放的问题,因为理论和实验结果之间的差异.
研究的目的:
- 实验研究SERS强度对各种金纳米结构 (纳米棒,纳米三角形,纳米星) 的局部等离子体共振 (LPR) 波长的依赖.
- 将实验SERS结果与理论预测进行比较,并评估不同激发激光波长 (633nm和785nm) 的影响.
- 分析纳米粒子形态 (1D,2D,3D) 和功能化对SERS性能在一系列LPR波长的影响.
主要方法:
- 金纳米棒 (AuNRs),金纳米三角形 (AuNTs) 和金纳米恒星 (AuNSTs) 被合成,它们的LPR波长通过化学蚀刻 (580-1020nm) 调整.
- 纳米粒子用Cy7.5和NBT进行了功能化,并使用633nm和785nm激光器测量了SERS强度在特定的拉曼转移 (940cm−1对于Cy7.5,1343cm−1对于NBT) 时.
- 电磁SERS增强因子是通过平均局部场强度来计算的,并与实验SERS等离子形状进行比较.
主要成果:
- 与激光波长相比,计算的SERS等离子体概况被红移,与633nm相比,785nm激发的计算EFs更高.
- 与NBT功能化的粒子相比,AuNR@Cy7.5和AuNT@Cy7.5的实验SERS信号显著更强 (35倍),而AuNST对两种功能化都有类似的反应.
- 观察到的SERS等离子体形状表现出扩大和偏离理论的四次数定律,在785nm激发后出现轻微的蓝色偏移,在633nm激发后出现红色偏移.
结论:
- 实验性SERS性能受到纳米粒子形态,功能和激发波长的影响,通常偏离简单的理论预测.
- 最大SERS信号的最佳LPR不仅取决于激光波长,而是包括粒子形状和激发能量在内的因素的复杂相互作用.
- 该研究强调了当前电磁理论在充分解释实验性SERS增强因素方面的局限性,并建议需要进一步改进.
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