Chemical Engineering Department, University of Louisville, Louisville, KY 40292, USA.
J Nanobiotechnology. 2011 May 10;9:16. doi: 10.1186/1477-3155-9-16.
When a fluorophore is placed in the vicinity of a metal nanoparticle possessing a strong plasmon field, its fluorescence emission may change extensively. Our study is to better understand this phenomenon and predict the extent of quenching and/or enhancement of fluorescence, to beneficially utilize it in molecular sensing/imaging.
Plasmon field intensities on/around gold nanoparticles (GNPs) with various diameters were theoretically computed with respect to the distance from the GNP surface. The field intensity decreased rapidly with the distance from the surface and the rate of decrease was greater for the particle with a smaller diameter. Using the plasmon field strength obtained, the level of fluorescence alternation by the field was theoretically estimated. For experimental studies, 10 nm GNPs were coated with polymer layer(s) of known thicknesses. Cypate, a near infrared fluorophore, was placed on the outermost layer of the polymer coated GNPs, artificially separated from the GNP at known distances, and its fluorescence levels were observed. The fluorescence of Cypate on the particle surface was quenched almost completely and, at approximately 5 nm from the surface, it was enhanced ~17 times. The level decreased thereafter. Theoretically computed fluorescence levels of the Cypate placed at various distances from a 10 nm GNP were compared with the experimental data. The trend of the resulting fluorescence was similar. The experimental results, however, showed greater enhancement than the theoretical estimates, in general. The distance from the GNP surface that showed the maximum enhancement in the experiment was greater than the one theoretically predicted, probably due to the difference in the two systems.
Factors affecting the fluorescence of a fluorophore placed near a GNP are the GNP size, coating material on GNP, wavelengths of the incident light and emitted light and intrinsic quantum yield of the fluorophore. Experimentally, we were able to quench and enhance the fluorescence of Cypate, by changing the distance between the fluorophore and GNP. This ability of artificially controlling fluorescence can be beneficially used in developing contrast agents for highly sensitive and specific optical sensing and imaging.
当荧光团置于具有强等离子体场的金属纳米颗粒附近时,其荧光发射可能会发生广泛变化。我们的研究旨在更好地理解这一现象,并预测荧光猝灭和/或增强的程度,以便在分子传感/成像中有益地利用它。
用不同直径的金纳米颗粒(GNPs)理论上计算了相对于 GNP 表面的距离的等离子体场强度。场强随距离表面的距离迅速下降,并且直径较小的颗粒下降速度更快。利用获得的等离子体场强度,理论上估计了场对荧光的改变程度。在实验研究中,用已知厚度的聚合物层涂覆 10nm 的 GNPs。将近红外荧光团 Cypate 置于聚合物涂覆的 GNPs 的最外层,人为地与颗粒保持已知距离,并观察其荧光水平。Cypate 在颗粒表面的荧光几乎完全猝灭,在距离表面约 5nm 处,增强约 17 倍。此后,水平下降。将 Cypate 置于距 10nm GNP 不同距离处的理论计算的荧光水平与实验数据进行了比较。产生的荧光趋势相似。然而,实验结果总体上显示出比理论估计更大的增强。实验中显示最大增强的 GNP 表面距离大于理论预测的距离,可能是由于两个系统的差异。
影响置于 GNP 附近的荧光团荧光的因素是 GNP 的尺寸、GNP 上的涂层材料、入射光和发射光的波长以及荧光团的固有量子产率。在实验中,我们能够通过改变荧光团与 GNP 之间的距离来猝灭和增强 Cypate 的荧光。这种人工控制荧光的能力可用于开发高灵敏度和特异性光学传感和成像的对比剂。