Department of Electrical and Computer Engineering, Boston University, Boston, Massachusetts, USA.
ACS Nano. 2011 Dec 27;5(12):9898-906. doi: 10.1021/nn203604v. Epub 2011 Nov 21.
The exciton dynamics for an ensemble of individual, suspended (6,5), single-walled carbon nanotubes revealed by single color E(22) resonant pump-probe spectroscopy for a wide range of pump fluences are reported. The optically excited initial exciton population ranges from approximately 5 to 120 excitons per ∼725 nm nanotube. At the higher fluences of this range, the pump-probe signals are no longer linearly dependent on the pump intensity. A single, predictive model is described that fits all data for two decades of pump fluences and three decades of delay times. The model introduces population loss from the optically active zero momentum E(22) state to the rest of the E(22) subband, which is dark due to momentum selection rules. In the single exciton limit, the E(11) dynamics are well described by a stretched exponential, which is a direct consequence of diffusion quenching from an ensemble of nanotubes of different lengths. The observed change in population relaxation dynamics as a function of increasing pump intensity is attributed to exciton-exciton Auger de-excitation in the E(11) subband and, to a lesser extent, in the E(22) subband. From the fit to the model, an average defect density 1/ρ = 150 nm and diffusion constants D(11) = 4 cm(2)/s and D(22) = 0.2 cm(2)/s are determined.
报道了通过单波长 E(22)共振泵浦探测光谱研究在宽泵浦强度范围内单个悬浮(6,5)单壁碳纳米管的激子动力学。光学激发的初始激子密度范围约为每个 ∼725nm 纳米管 5 到 120 个激子。在该范围内的较高强度下,泵浦探测信号不再与泵浦强度呈线性关系。描述了一个单一的、可预测的模型,该模型适用于两个数量级的泵浦强度和三个数量级的延迟时间的所有数据。该模型引入了从光活性零动量 E(22)态到其余 E(22)子带的种群损失,由于动量选择规则,E(22)子带是暗的。在单激子极限下,E(11)动力学很好地由拉伸指数描述,这是由于不同长度的纳米管的集合中的扩散猝灭直接导致的。观察到的随着泵浦强度增加而变化的种群弛豫动力学归因于 E(11)子带和在较小程度上的 E(22)子带中的激子-激子俄歇退激发。从对模型的拟合中,确定了平均缺陷密度 1/ρ=150nm 和扩散常数 D(11)=4cm(2)/s 和 D(22)=0.2cm(2)/s。