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Near-infrared surface plasmon resonance measurements of ultrathin films. 1. Angle shift and SPR imaging experiments

机译:超薄膜的近红外表面等离子体共振测量。 1.角度偏移和SPR成像实验

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The application of surface plasmon resonance (SPR) measurements to the study of ultrathin organic and inorganic films adsorbed onto gold surfaces utilizing near-infrared (NIR) excitation from 800 to 1152 mn is described. SPR scanning angle measurements of film thickness are demonstrated at 814 and 1152 nm using low-power diode and HeNe laser sources, respectively. Several advantages of SPR in the NIR are noted. The in situ reflectivity versus angle of incidence curves sharpen greatly (as compared to 632.8 nm) at longer wavelengths so that there is no loss in sensitivity in the measurement of film thickness despite a doubling of the excitation wavelength. The sharper resonance and longer wavelengths also allow for the measurement of thicker films. Examples of SPR thickness measurements for self-assembled alkanethiol monolayers and composite biopolymer/SiO2 nanoparticle electrostatic multilayer films are given. SPR imaging experiments are also performed at various NIR wavelengths using an incoherent white light source and narrow band-pass filters. The incoherent white light source eliminates laser fringes that have been observed in previous SPR imaging experiments, and the use of narrow band-pass filters allows for the easy selection and variation of excitation wavelength. The narrowness of the reflectivity versus angle curves leads to greater contrast in NIR SPR images compared to the same features examined with excitation from visible light. The combination of these changes results in nearly 1 order of magnitude enhancement in the SPR differential reflectivity image, indicating that SPR imaging is best conducted with incoherent NIR excitation. One disadvantage of using NIR wavelengths for SPR imaging is that the surface plasmon propagation length increases in the NIR so that the lateral image resolution is reduced; however, image features larger than 50 mu m can easily be resolved. A NIR SPR image of a DNA array onto which single-stranded DNA binding protein has bound is shown as an example of how NIR SPR imaging experiments have sufficient sensitivity to monitor DNA-protein interactions. [References: 36]
机译:描述了表面等离振子共振(SPR)测量在利用800至1152 mn的近红外(NIR)激发研究吸附在金表面的超薄有机和无机膜中的应用。使用低功率二极管和HeNe激光源分别在814和1152 nm处证明了膜厚度的SPR扫描角测量。指出了NIR中SPR的几个优点。在更长的波长处,原位反射率与入射角的关系曲线大大变尖(与632.8 nm相比),因此,即使激发波长加倍,在膜厚测量中也不会损失灵敏度。共振更尖锐,波长更长,也可以测量较厚的薄膜。给出了自组装烷硫醇单层和复合生物聚合物/ SiO2纳米粒子静电多层膜的SPR厚度测量示例。使用非相干白光源和窄带通滤光片,还可以在各种NIR波长下进行SPR成像实验。非相干白光源消除了先前SPR成像实验中观察到的激光条纹,并且使用窄带通滤光片可以轻松选择和改变激发波长。与可见光激发下检测到的相同特征相比,反射率与角度曲线的窄度导致NIR SPR图像具有更大的对比度。这些变化的组合导致SPR差分反射率图像中的幅度提高了将近1个数量级,表明SPR成像最好在非相干NIR激发下进行。使用NIR波长进行SPR成像的一个缺点是,表面等离激元传播长度会在NIR中增加,从而降低了横向图像分辨率。但是,大于50微米的图像特征很容易解决。显示了单链DNA结合蛋白已结合到其上的DNA阵列的NIR SPR图像,作为NIR SPR成像实验如何具有足够的灵敏度来监视DNA-蛋白质相互作用的示例。 [参考:36]

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