Department of Chemistry, Texas A&M University, College Station, Texas 77842, USA.
ACS Nano. 2012 Jan 24;6(1):583-91. doi: 10.1021/nn204452e. Epub 2012 Jan 10.
Dynamics of energy transfer and charge carrier localization in Mn-doped CdS/ZnS core/shell nanocrystals correlated with doping location and concentration are studied via transient absorption measurement of exciton relaxation dynamics. The strong dependence of exciton-Mn energy transfer rate on doping location was directly resolved in the transient bleach recovery and electron intraband absorption data by using layer-by-layer synthesized Mn-doped nanocrystals. With 1.2 nm decrease in doping radius in the ZnS shell, energy transfer rate increases by 6 fold. We identified that hole trapping is the major competing process that inhibits the energy transfer in Mn-doped CdS/ZnS nanocrystals. From the branching ratio of the energy transfer and hole trapping, combined with luminescence quantum yield measurement, we also obtained doping location-dependent radiative relaxation quantum yield of Mn(2+) ions that is as high as 0.95.
通过瞬态吸收测量激子弛豫动力学,研究了与掺杂位置和浓度相关的 Mn 掺杂 CdS/ZnS 核/壳纳米晶体中能量转移和电荷载流子局域化的动力学。通过使用逐层合成的 Mn 掺杂纳米晶体,在瞬态漂白恢复和电子内带吸收数据中直接解析了激子-Mn 能量转移速率对掺杂位置的强烈依赖性。随着 ZnS 壳中掺杂半径减小 1.2nm,能量转移速率增加了 6 倍。我们确定空穴捕获是主要的竞争过程,它抑制了 Mn 掺杂 CdS/ZnS 纳米晶体中的能量转移。根据能量转移和空穴捕获的分支比,结合荧光量子产率测量,我们还获得了与掺杂位置相关的 Mn(2+)离子的辐射弛豫量子产率高达 0.95。