利用N型半导体纳米材料抑制单量子点的荧光闪烁特性

利用N型半导体纳米材料氧化铟锡(ITO)作为单CdSe/ZnS量子点的基质来抑制单量子点的荧光闪烁特性. 实验采用激光扫描共聚焦显微成像系统测量了单量子点荧光的亮、暗态持续时间的概率密度分布的指数截止的幂律特性, 并与直接吸附在SiO₂玻片上的单CdSe/ZnS量子点的荧光特性进行比较. 研究发现处于ITO中的单量子点比SiO₂玻片上的单量子点荧光亮态持续时间提高两个数量级, 掺杂于ITO中的单量子点的荧光寿命约减小为SiO₂玻片上的单量子点的荧光寿命的41%, 并且寿命分布宽度变小50%.

Suppression of the blinking of single QDs by using an N-type semiconductor nanomaterial

Single quantum dots (QDs) always exhibit strong blinking in fluorescence intensity when they are on some inert substrates. The blinking activity is attributed to the photoinduced charging of QDs by electron transfer (ET) to trap states in QDs and the surrounding matrix, which has been considered as an undesirable property in many applications. Here, we use N-doped indium tin oxide (ITO) semiconductor nanoparticles to suppress fluorescence blinking activity of single CdSe/ZnS core/shell QDs. The fluorescence characteristics of single QDs in ITO and on SiO₂ cover glass are measured by a laser scanning confocal fluorescence microscopy, respectively. It is found that the on-and off-state probability densities of QDs on different substrates both can be fit by a truncated power law. Blinking rates for single QDs on glass and in ITO are also calculated. By contrast, single QDs doped in ITO show that their blinking rate and fluorescence lifetime both decrease. The on-state probability density of single QDs in ITO is approximately two orders of magnitude higher than that of QDs on SiO₂ cover glass. It means that single QDs doped in ITO have a longer time to be on-state. Because the Fermi level in QDs is lower than in ITO, when they are in contact, electrons in ITO will transfer to QDs. As a result, the equilibration of their Fermi levels leads to the formation of negatively charged QDs. These electrons fill in the holes of QDs shell and enhance the on-state probability of QDs. Fluorescence decays of single QDs on glass and in ITO are measured by TAC/MCA, and they can be fit by biexponential function. The two lifetime values correspond to the single exciton lifetime and biexciton lifetime of QDs, respectively. It is worth noting that the distribution of the amplitude weighted average lifetime for single QDs in ITO is approximately 41% of that for single QDs on SiO₂ cover glass and its full width at half maximum (FWHM) is changed to 50%. For the conduction band potential of QDs is higher than that of ITO, which contributes to photoinduced interfacial electron transfer from QDs to ITO and leads to the increase of nonradiative transition. These indicate that ITO can reduce single exciton and biexciton lifetime of QDs. The study demonstrates that ITO can effectively suppress the blinking activity of QDs.