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Enhancing Raman signals through electromagnetic hot zones induced by magnetic dipole resonance of metal-free nanoparticles

机译:通过无金属型纳米粒子的磁性偶极子谐振诱导的电磁热区增强拉曼信号

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In this study, we found that the large area of electromagnetic field hot zone induced through magnetic dipole resonance of metal-free structures can greatly enhance Raman scattering signals. The magnetic resonant nanocavities, based on high-refractive-index silicon nanoparticles (SiNPs), were designed to resonate at the wavelength of the excitation laser of the Raman system. The well-dispersed SiNPs that were not closely packed displayed significant magnetic dipole resonance and gave a Raman enhancement per unit volume of 59 347. The hot zones of intense electric field were generated not only within the nonmetallic NPs but also around them, even within the underlying substrate. We observed experimentally that gallium nitride (GaN) and silicon carbide (SiC) surfaces presenting very few SiNPs (coverage: <0.3%) could display significantly enhanced (>50%) Raman signals. In contrast, the Raman signals of the underlying substrates were not enhanced by gold nanoparticles (AuNPs), even though these NPs displayed a localized surface plasmon resonance (LSPR) phenomenon. A comparison of the areas of the electric field hot zones (E-2 > 10) generated by SiNPs undergoing magnetic dipole resonance with the electric field hot spots (E-2 > 10) generated by AuNPs undergoing LSPR revealed that the former was approximately 70 times that of the latter. More noteworthily, the electromagnetic field hot zone generated from the SiNP is able to extend into the surrounding and underlying media. Relative to metallic NPs undergoing LSPR, these nonmetallic NPs displaying magnetic dipole resonance were more effective at enhancing the Raman scattering signals from analytes that were underlying, or even far away from, them. This application of magnetic dipole resonance in metal-free structures appears to have great potential for use in developing next-generation techniques for Raman enhancement.
机译:在这项研究中,我们发现,通过无金属结构的磁偶极子磁共振感应电磁场热区的大面积可大大增强拉曼散射信号。磁谐振纳米空腔,基于高折射率硅纳米颗粒(SiNPs),被设计为在共振拉曼系统的激发激光的波长。那些没有密集的良好分散SiNPs显示显著磁偶极共振,给拉曼增强每单位体积的59个347强电场的热区不仅非金属纳米颗粒内,但也他们身边,即使在产生下面的衬底。我们通过实验观察到,氮化镓(GaN)和碳化硅(SiC)表面呈现非常少SiNPs(覆盖率<0.3%)可能显示显著增强(> 50%)的拉曼信号。与此相反,底层基片的拉曼信号不是由金粒子(AuNPs)增强,即使这些NP显示的局域型表面等离子体共振(LSPR)现象。通过经历磁偶极共振通过经历LSPR的AuNP产生的电场的热点(E-2> 10)SiNPs产生的电场的热区(E-2> 10)的面积的比较显示,前者约为70倍后者的。更noteworthily,从SINP产生的电磁场热区能够延伸到周围和下层媒质。相对于接受LSPR金属纳米粒子,这些纳米粒子非金属显示磁偶极子共振是在不同于从,它们底层,或者甚至远分析物增强拉曼散射信号更有效。磁偶极子共振的无金属结构此应用程序似乎有很大的潜力,在开发下一代技术拉曼增强使用。

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