Department of Chemistry, 590 Commonwealth Avenue, Boston University, Boston, Massachusetts 02215, United States.
J Phys Chem A. 2011 Apr 28;115(16):3917-23. doi: 10.1021/jp108345t. Epub 2011 Jan 11.
Highly nonlinear pump fluence dependence was observed in the ultrafast one-color pump-probe responses excited by 38 fs pulses resonant with the E(22) transition in a room-temperature solution of (6,5) carbon nanotubes. The differential probe transmission (ΔT/T) at the peak of the pump-probe response (τ = 20 fs) was measured for pump fluences from ∼10(13) to 10(17) photons/pulse cm(2). The onset of saturation is observed at ∼2 × 10(15) photons/pulse cm(2) (∼8 × 10(5) excitons/cm). At pump fluences >4 × 10(16) photons/pulse cm(2) (∼1.6 × 10(6) excitons/cm), ΔT/T decreases as the pump fluence increases. Analogous signal saturation behavior was observed for all measured probe delays. Despite the high exciton density at saturation, no change in the E(22) population decay rate was observed at short times (<300 fs). The pump probe signal was modeled by a third-order perturbation theory treatment that includes the effects of inhomogeneous broadening. The observed ΔT/T signal is well-fit by a pump-fluence-dependent dephasing rate linearly dependent on the number of excitons created by the pump pulse. Therefore, the observed nonlinear pump intensity dependence is attributed to the effects of quasi-elastic exciton-exciton interactions on the dephasing rates of single carbon nanotubes. The low fluence total dephasing time is 36 fs, corresponding to a homogeneous width of 36 meV (290 cm(-1)), and the derived E(22) inhomogeneous width is 68 meV (545 cm(-1)). These results are contrasted with photon-echo-derived parameters for the E(11) transition.
在室温下(6,5)碳纳米管溶液中,用 38fs 脉冲激发与 E(22)跃迁共振的单波长泵浦-探测响应中,观察到了非线性泵浦光强的高度依赖性。在探测延迟时间为 20fs 的泵浦-探测响应的峰值处,测量了从约 10(13)到 10(17)光子/脉冲·cm(-2)的泵浦光强下的微分探测透过率(ΔT/T)。在约 2×10(15)光子/脉冲·cm(-2)(约 8×10(5)激子/cm)处观察到了饱和的起始点。在泵浦光强>4×10(16)光子/脉冲·cm(-2)(约 1.6×10(6)激子/cm)时,随着泵浦光强的增加,ΔT/T 减小。在所有测量的探测延迟时间下,都观察到了类似的信号饱和行为。尽管在饱和时激子密度很高,但在短时间(<300fs)内没有观察到 E(22)布居衰减率的变化。通过三阶微扰理论处理,考虑了非均匀展宽的影响,对泵浦探测信号进行了建模。观察到的 ΔT/T 信号与由泵浦脉冲产生的激子数量有关的、与泵浦光强相关的退相速率线性拟合良好。因此,观察到的非线性泵浦强度依赖性归因于准弹性激子-激子相互作用对单个碳纳米管退相速率的影响。低光强总退相时间为 36fs,对应于均匀宽度 36meV(290cm(-1)),并推导出 E(22)非均匀宽度为 68meV(545cm(-1))。这些结果与光子回波得出的 E(11)跃迁参数形成对比。