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首页> 外文期刊>ACS nano >Intensity-dependent exciton dynamics of (6,5) single-walled carbon nanotubes: Momentum selection rules, diffusion, and nonlinear interactions
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Intensity-dependent exciton dynamics of (6,5) single-walled carbon nanotubes: Momentum selection rules, diffusion, and nonlinear interactions

机译:(6,5)单壁碳纳米管的强度依赖激子动力学:动量选择规则,扩散和非线性相互作用

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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/φ = 150 nm and diffusion constants D _(11) = 4 cm~2/s and D_(22) = 0.2 cm~2/s are determined.
机译:报告了由单个E_(22)共振泵浦探针光谱学揭示的单个,悬浮的(6,5)单壁碳纳米管集合体在大范围的泵浦注量中的激子动力学。每〜725 nm纳米管的光激发初始激子总数约为5至120个激子。在此范围的较高通量下,泵浦探针信号不再线性地取决于泵浦强度。描述了一个单一的预测模型,该模型适合泵浦注量的二十年和延迟时间的三十年的所有数据。该模型将人口损失从旋光零动量E_(22)状态引入到E_(22)子带的其余部分,该子带由于动量选择规则而变暗。在单个激子极限中,E_(11)动力学很好地通过拉伸指数来描述,这是来自不同长度纳米管集合的扩散猝灭的直接结果。 E_(11)子带中的激子-激子俄歇去激励,并且在较小程度上,E_(22)子带中观察到的随弛豫强度增加而变化的种群弛豫动力学变化。根据模型拟合,确定平均缺陷密度1 /φ= 150 nm,扩散常数D _(11)= 4 cm〜2 / s,D_(22)= 0.2 cm〜2 / s。

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