Maity Partha, Debnath Tushar, Chopra Uday, Ghosh Hirendra Nath
Radiation and Photochemistry Division, Bhabha Atomic Research Centre, Mumbai-400085, India.
Nanoscale. 2015 Feb 14;7(6):2698-707. doi: 10.1039/c4nr05829a.
Ultrafast cascading hole and electron transfer dynamics have been demonstrated in a CdS/CdTe type II core-shell sensitized with Br-PGR using transient absorption spectroscopy and the charge recombination dynamics have been compared with those of CdS/Br-PGR composite materials. Steady state optical absorption studies suggest that Br-PGR forms strong charge transfer (CT) complexes with both the CdS QD and CdS/CdTe core-shell. Hole transfer from the photo-excited QD and QD core-shell to Br-PGR was confirmed by both steady state and time-resolved emission spectroscopy. Charge separation was also confirmed by detecting electrons in the conduction band of the QD and the cation radical of Br-PGR as measured from femtosecond transient absorption spectroscopy. Charge separation in the CdS/Br-PGR composite materials was found to take place in three different pathways, by transferring the photo-excited hole of CdS to Br-PGR, electron injection from the photo-excited Br-PGR to the CdS QD, and direct electron transfer from the HOMO of Br-PGR to the conduction band of the CdS QD. However, in the CdS/CdTe/Br-PGR system hole transfer from the photo-excited CdS to Br-PGR and electron injection from the photo-excited Br-PGR to CdS take place after cascading through the CdTe shell QD. Charge separation also takes place via direct electron transfer from the Br-PGR HOMO to the conduction band of CdS/CdTe. Charge recombination (CR) dynamics between the electron in the conduction band of the CdS QD and the Br-PGR cation radical were determined by monitoring the bleach recovery kinetics. The CR dynamics were found to be much slower in the CdS/CdTe/Br-PGR system than in the CdS/Br-PGR system. The formation of the strong CT complex and the separation of charges cascading through the CdTe shell help to slow down charge recombination in the type II regime.
利用瞬态吸收光谱法,在以Br-PGR敏化的CdS/CdTe II型核壳结构中证实了超快级联空穴和电子转移动力学,并将电荷复合动力学与CdS/Br-PGR复合材料的进行了比较。稳态光吸收研究表明,Br-PGR与CdS量子点(QD)和CdS/CdTe核壳结构均形成了强电荷转移(CT)复合物。稳态和时间分辨发射光谱均证实了光激发的量子点和量子点核壳结构中的空穴向Br-PGR的转移。通过飞秒瞬态吸收光谱测量,在量子点导带中检测到电子以及Br-PGR的阳离子自由基,也证实了电荷分离。发现CdS/Br-PGR复合材料中的电荷分离通过三种不同途径发生:将光激发的CdS空穴转移至Br-PGR、光激发的Br-PGR向CdS量子点注入电子、以及Br-PGR的最高占据分子轨道(HOMO)向CdS量子点导带的直接电子转移。然而,在CdS/CdTe/Br-PGR体系中,光激发的CdS向Br-PGR的空穴转移以及光激发的Br-PGR向CdS的电子注入是在通过CdTe壳层量子点级联之后发生的。电荷分离也通过Br-PGR HOMO向CdS/CdTe导带的直接电子转移发生。通过监测漂白恢复动力学,确定了CdS量子点导带中的电子与Br-PGR阳离子自由基之间的电荷复合(CR)动力学。发现CdS/CdTe/Br-PGR体系中的CR动力学比CdS/Br-PGR体系中的慢得多。强CT复合物的形成以及通过CdTe壳层的电荷分离有助于减缓II型体系中的电荷复合。