A comparative study of anti-Stokes shift under stimulated Rayleigh-Mie scattering in suspensions of Ag nanoparticles obtained in plasma discharge in liquid under ultrasonic cavitation

N. Bulychev, A. Erokhin, M. Kazaryan
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Abstract

Stimulated Rayleigh–Mie scattering (SRMS) in two-photon absorption liquids is realized by a Fourier transform-limited pulsed Nd-glass laser. For the first time, we have measured anti-Stokes spectral shifts of SRMS in toluene and hexane colloids of Ag nanoparticles, as well as in pure toluene. The suspensions are prepared in the plasma discharge excited in a liquid exposed to an intense ultrasonic field above the cavitation threshold. This novel technique has been developed for the synthesis of various nano-sized materials; it provides silver nanoparticles suspensions with controlled narrow distribution of the particle size. Ultrasonic cavitation results in a drastic change in the physical properties of the liquid, providing specific conditions in the electrical discharge plasma. Ag nanoparticles with 1-2 nm radii in toluene and hexane are obtained from silver electrodes under these specific conditions and acquire unique surface characteristics which prevent them from secondary agglomeration. The values of anti-Stokes spectral shifts of SRMS appreciably exceed the Rayleigh line width in those liquids. The four-wave mixing method is applied both experimentally and theoretically to display the process as Rayleigh-induced parametric generation. We show that the amplification effect is provided predominantly by thermally induced coherent polarization oscillations, while an interference-assisted thermal grating provides formation of a self-induced optical cavity inside the interaction region.
超声空化条件下等离子体放电制备银纳米粒子悬浮液中受激瑞利-米氏散射下反斯托克斯位移的比较研究
利用限制傅里叶变换的脉冲钕玻璃激光器实现了双光子吸收液体中的受激瑞利-米氏散射。我们首次在甲苯和银纳米颗粒的己烷胶体以及纯甲苯中测量了SRMS的反斯托克斯光谱位移。该悬浮液是在暴露于高于空化阈值的强超声场的液体中激发的等离子体放电中制备的。这种新技术已发展为各种纳米材料的合成;它提供了银纳米颗粒悬浮液与控制窄分布的粒度。超声空化导致液体物理性质的剧烈变化,在放电等离子体中提供特定的条件。在这些特定条件下,银电极在甲苯和己烷中获得了半径为1 ~ 2 nm的银纳米颗粒,并获得了独特的表面特征,防止了银纳米颗粒的二次团聚。在这些液体中,SRMS的反斯托克斯谱移值明显超过瑞利谱宽。从实验和理论两方面应用四波混频方法,表明该过程为瑞利诱导的参数产生过程。我们发现,放大效应主要是由热诱导的相干偏振振荡提供的,而干涉辅助热光栅在相互作用区域内提供了自诱导光腔的形成。
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