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Hyper-Rayleigh scattering and multiphoton fluorescence of nanoscale CdS colloids in water

机译:纳米级CDS胶体在水中的Hyper-Rayleigh散射和多光子荧光

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Optical nonlinearities of semiconductor nanoparticles are of great interest recently. Here the hyper-Rayleigh scattering (HRS) technique is used to measure the second-order nonlinear optical (NLO) response of nanoscale CdS Colloids with different surfaces in water. It shows that the HRS signals for CdS Colloids are very strong. The 'per particle' first-order hyperpolarizability values $beta are estimated to fall in the range of 10$+$MIN@26$/ esu, and 'per CdS unit' are in the range of 10$+$MIN@28$/ esu which is very large. And the $beta values are different for CdS nanoparticles with different surfaces. Further studies show that the CdS/SC(NH$-2$/)$-2$/ nanoparticle has strong multi- photon fluorescence (MPF) emission under the radiation of 1064 nm so the large signal at 532 nm is mainly from the MPF. But for Cd$+2$PLU$/-rich and S$+2$/-rich CdS nanoparticles the MPF are relatively weaker at 532 nm. These experiments reveal that the HRS or MPF signals are very sensitive to the changes of the nanoparticle surface and can provide useful information about the nanoparticle/solution interface. They also give the evidences proving that surface termination of the crystalline lattice that creates a conditions of non-centrosymmetry is contributing to the large $beta value for CdS nanoparticles.
机译:半导体纳米粒子的光学非线性是最近的极大兴趣。在这里,超瑞利散射(HRS)技术被用于测量所述第二阶非线性与水不同的表面的纳米级的CdS胶体的光学(NLO)响应。这表明,硫化镉胶体的HRS信号非常强。在“每个颗粒”第一阶超极化率值$的β估计落在10 $ + $ MIN @ 26 $ / ESU,和“每CDS单元”是在10 $ + $ MIN @ 28 $的范围的范围内/ ESU这是非常大的。 $ Beta值对于具有不同表面的CDS纳米粒子不同。进一步的研究表明,在CdS / SC(NH $ -2 $ /)$ - 1064nm的辐射下$ 2 /纳米颗粒具有强的多光子荧光(MPF)发射,从而在532nm处的大的信号主要来自MPF 。但对于镉$ + 2 $ PLU $ / - 丰富和S $ + $ 2 / - 丰富的CdS纳米强积金是在532nm处相对较弱。这些实验表明,该HRS或MPF信号对纳米粒子表面的变化非常敏感,并且可以提供关于纳米颗粒/溶液界面的有用信息。他们也给了证据证明造成非中心对称的条件促成的CD纳米颗粒大$测试值晶格的那个表面终止。

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