Rout Sangeeta, Qi Zhen, Petrosyan Ludvig S, Shahbazyan Tigran V, Biener Monika M, Bonner Carl E, Noginov Mikhail A
Center for Materials Research, Norfolk State University, Norfolk, VA 23504, USA.
Lawrence Livermore National Laboratory, Livermore, CA 94550, USA.
Nanomaterials (Basel). 2020 Oct 27;10(11):2135. doi: 10.3390/nano10112135.
We have studied emission kinetics of HITC laser dye on top of glass, smooth Au films, and randomly structured porous Au nanofoams. The observed concentration quenching of luminescence of highly concentrated dye on top of glass (energy transfer to acceptors) and the inhibition of the concentration quenching in vicinity of smooth Au films were in accord with our recent findings. Intriguingly, the emission kinetics recorded in different local spots of the Au nanofoam samples had a spread of the decay rates, which was large at low dye concentrations and became narrower with increase of the dye concentration. We infer that in different subvolumes of Au nanofoams, HITC molecules are coupled to the nanofoams weaker or stronger. The inhibition of the concentration quenching in Au nanofoams was stronger than on top of smooth Au films. This was true for all weakly and strongly coupled subvolumes contributing to the spread of the emission kinetics. The experimental observations were explained using theoretical model accounting for change in the Förster radius caused by the strong energy transfer to metal.
我们研究了HITC激光染料在玻璃、光滑金膜和随机结构的多孔金纳米泡沫上的发射动力学。观察到玻璃表面高浓度染料发光的浓度猝灭(能量转移给受体)以及光滑金膜附近浓度猝灭的抑制与我们最近的发现一致。有趣的是,在金纳米泡沫样品的不同局部位置记录的发射动力学具有衰减率的分散,在低染料浓度时较大,并且随着染料浓度的增加而变窄。我们推断,在金纳米泡沫的不同子体积中,HITC分子与纳米泡沫的耦合有强有弱。金纳米泡沫中浓度猝灭的抑制比光滑金膜表面更强。对于导致发射动力学分散的所有弱耦合和强耦合子体积都是如此。利用考虑到由于向金属的强能量转移导致的福斯特半径变化的理论模型对实验观察结果进行了解释。