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Dissecting charge relaxation pathways in CdSe/CdS nanocrystals using femtosecond two-dimensional electronic spectroscopy

机译:解剖电荷弛豫通路CdSe / cd使用飞秒二维纳米晶体电子光谱

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Exciton relaxation dynamics of CdSe and quasi-type-II CdSe/CdS core/shell nanocrystals were examined using femtosecond two-dimensional electronic spectroscopy (2DES). The use of 2DES allowed for determination of structure-specific and state-resolved carrier dynamics for CdSe nanocrystals formed with five, or fewer, CdS passivation monolayers (ML). For CdSe and CdSe/CdS nanocrystals formed with one through three MLs of CdS, excitation using broad bandwidth femtosecond visible laser pulses generated electron-hole pairs among the |X-1 > = 2.14 eV and |X-2 > = 2.27 eV exciton states. For both excitations, the electron is promoted to the lowest energy excited (1S(c)) conduction-band state and the hole is in the 1S(3/2) (X-1) or 2S(3/2) (X-2) valence-band state. Therefore, the relaxation dynamics of the hot hole were isolated by monitoring the-time-dependent amplitude of 2DES cross peaks. The time constant for hot hole relaxation within the CdSe valence band was 150 +/- 45 fs. Upon passivation by CdS, this hole relaxation time constant increased to 170 +/- 30 fs (CdSe/CdS-3ML). This small increase was attributed to the formation of a graded, or alloyed, interfacial region that precedes the growth of a uniform CdS capping layer. The small increase in hole relaxation time reflects the larger nanocrystal volume of the CdSe/CdS system with respect to the CdSe nanocrystal core. In contrast, the dynamics of larger core/shell nanocrystals (>= 4ML CdS) exhibited a picosecond buildup in 2DES cross-peak amplitude. This time-dependent response was attributed to interfacial hole transfer from CdS to CdSe valence-band states. Importantly, the 2DES data distinguish CdSe exciton relaxation from interfacial carrier transfer dynamics. In combination, isolation of structurally well-defined nanocrystals and state-resolved 2DES can be used to examine directly the influence of nanoscale structural modifications on electronic carrier dynamics, which are critical for developing nanocluster-based photonic devices.
机译:激子弛豫动力学CdSe和检查使用飞秒二维电子光谱(2 des)。允许structure-specific的决心并为CdSe state-resolved载体动力学纳米晶体形成有5个或更少,cd钝化层(ML)。与一个通过CdSe / CdS纳米晶体形成三MLs的cd,激发使用广泛带宽的飞秒激光脉冲可见产生电子空穴对在| x - 1 > =2.14 eV和| x - 2 > = 2.27 eV激子态。作用,电子将提升能量最低兴奋传导带(1 s (c))州和孔在1 s (x - 1)或(3/2)2 s (3/2) (x - 2)价带状态。弛豫动力学热洞被孤立通过监测the-time-dependent振幅2 des交叉峰。放松在CdSe价带是150年+ / - 45 fs。弛豫时间常数增加到170 + / - 30fs (CdSe / CdS-3ML)。归因于一个分级的形成,或合金,界面区域之前发展一个统一的cd覆盖层。弛豫时间反映了增加洞更大的纳米晶体的体积CdSe / cd系统关于CdSe纳米晶体的核心。相比之下,更大的核/壳的动力纳米晶体(> = 4毫升CdS)展出微微秒积聚在2交叉峰的幅度。是由于时间响应从cd转移到CdSe界面洞价带。区分CdSe激子放松界面载波传输动力学。组合,隔离结构定义良好的纳米晶体和state-resolved 2 des可以直接用于检查的影响在电子纳米结构修改航空动力,这是至关重要的发展nanocluster-based光子设备。

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