Kilina Svetlana, Tretiak Sergei, Doorn Stephen K, Luo Zhengtang, Papadimitrakopoulos Fotios, Piryatinski Andrei, Saxena Avadh, Bishop Alan R
Theoretical Division, Center for Nonlinear Studies, and Center for Integrated Nanotechnologies, Los Alamos National Laboratory, Los Alamos, NM 87545, USA.
Proc Natl Acad Sci U S A. 2008 May 13;105(19):6797-802. doi: 10.1073/pnas.0711646105. Epub 2008 May 7.
Polarization of low-lying excitonic bands in finite-size semiconducting single-walled carbon nanotubes (SWNTs) is studied by using quantum-chemical methodologies. Our calculations elucidate properties of cross-polarized excitons, which lead to the transverse optical absorption of nanotubes and presumably couple to intermediate-frequency modes recently observed in resonance Raman excitation spectroscopy. We identify up to 12 distinct excitonic transitions below the second fundamental band associated with the E(22) van Hove singularity. Calculations for several chiral SWNTs distinguish the optically active "bright" excitonic band polarized parallel to the tube axis and several optically "weak" cross-polarized excitons. The rest are optically (near) forbidden "dark" transitions. An analysis of the transition density matrices related to excitonic bands provides detailed information about delocalization of excitonic wavefunction along the tube. Utilization of the natural helical coordinate system accounting for the tube chirality allows one to disentangle longitudinal and circumferential components. The distribution of the transition density matrix along a tube axis is similar for all excitons. However, four parallel-polarized excitons associated with the E(11) transition are more localized along the circumference of a tube, compared with others related to the E(12) and E(21) cross-polarized transitions. Calculated splitting between optically active parallel- and cross-polarized transitions increases with tube diameter, which compares well with experimental spectroscopic data.
利用量子化学方法研究了有限尺寸半导体单壁碳纳米管(SWNTs)中低能激子带的极化。我们的计算阐明了交叉极化激子的性质,这导致了纳米管的横向光吸收,并可能与最近在共振拉曼激发光谱中观察到的中频模式耦合。我们在与E(22)范霍夫奇点相关的第二基本带以下识别出多达12个不同的激子跃迁。对几种手性单壁碳纳米管的计算区分了平行于管轴极化的光学活性“亮”激子带和几种光学“弱”交叉极化激子。其余的是光学(近)禁戒的“暗”跃迁。对与激子带相关的跃迁密度矩阵的分析提供了关于激子波函数沿管的离域的详细信息。利用考虑管手性的自然螺旋坐标系可以区分纵向和圆周分量。所有激子沿管轴的跃迁密度矩阵分布相似。然而,与E(11)跃迁相关的四个平行极化激子在管的圆周上比与E(12)和E(21)交叉极化跃迁相关的其他激子更局域化。计算得到的光学活性平行极化和交叉极化跃迁之间的分裂随管直径增加,这与实验光谱数据吻合得很好。