National Renewable Energy Laboratory, 1617 Cole Boulevard, Golden, Colorado 80401, United States.
Nano Lett. 2011 Nov 9;11(11):4923-31. doi: 10.1021/nl202869z. Epub 2011 Oct 19.
Femtosecond cross-polarized transient grating (CPTG) and polarization anisotropy were used to probe the extent of electronic delocalization in CdSe/CdS quantum rod heterostructures (QRH) with a "dot-in-rod" geometry. The alignment of the bulk valence and conduction band edges of CdSe and CdS suggest a "type I" band configuration, leading to localization of both the electron and hole on the CdSe seed, but size quantization effects make the distinction less clear. Photoexcited electrons in 2.1 and 2.9 nm diameter structures have considerable excess kinetic energy above the CdS conduction band and show clear evidence of electron delocalization into the surrounding shell. However, the dependence of the CPTG decay rate on aspect ratio for 2.9 nm seeded QRHs is minimal, suggesting that the delocalization is mostly isotropic (i.e., not preferentially along the rod length). The rates for the 2.1 and 2.9 nm QRHs fall in line with expected trends based on effective exciton size. The 4.2 nm diameter structures also lack any rod length dependence of the CPTG decay and instead exhibit a biexponential decay that is indicative of coupled pathways for fine structure relaxation, likely due to anisotropic interfacial strain. CPTG is found to serve as a unique tool for determining charge transfer and delocalization in nanoheterostructures, which can rarely be predicted accurately from examination of bulk band offsets.
飞秒交叉偏振瞬态光栅 (CPTG) 和偏振各向异性被用来探测具有“点在棒”几何形状的 CdSe/CdS 量子棒异质结构 (QRH) 中电子离域的程度。CdSe 和 CdS 的体价带和导带边缘的排列表明了一种“类型 I”能带结构,导致电子和空穴都定域在 CdSe 核上,但尺寸量子化效应使得这种区分不那么明显。在 2.1 和 2.9nm 直径结构中,光激发的电子具有相当大的过剩动能,超过了 CdS 导带,并且清楚地表明电子离域到周围的壳层中。然而,2.9nm 种核 QRH 的 CPTG 衰减速率对纵横比的依赖性很小,这表明离域主要是各向同性的(即,不是优先沿棒的长度)。2.1 和 2.9nm QRH 的速率符合基于有效激子尺寸的预期趋势。4.2nm 直径的结构也没有 CPTG 衰减的任何棒长依赖性,而是表现出双指数衰减,这表明精细结构弛豫的耦合途径,可能是由于各向异性的界面应变。CPTG 被发现是一种确定纳米异质结构中电荷转移和离域的独特工具,从体带隙偏移的检查中很难准确预测。