Department of Chemistry, University of California, Riverside, Riverside, California 92521, USA.
J Chem Phys. 2011 Dec 7;135(21):214508. doi: 10.1063/1.3664630.
The excited state dynamics of polycrystalline tetracene films are studied using femtosecond transient absorption in combination with picosecond fluorescence, continuing work reported in an earlier paper [J. J. Burdett, A. M. Muller, D. Gosztola, and C. J. Bardeen, J. Chem. Phys. 133, 144506 (2010)]. A study of the intensity dependence of the singlet state decay is conducted to understand the origins of the discrepancy between the broadband transient absorption and fluorescence experiments seen previously. High-sensitivity single channel transient absorption experiments allow us to compare the transient absorption dynamics to the fluorescence dynamics measured at identical laser fluences. At high excitation densities, an exciton-exciton annihilation rate constant of 1 × 10(-8) cm(3) s(-1) leads to rapid singlet decays, but at excitation densities of 2 × 10(17) cm(-3) or less the kinetics of the transient absorption match those of the fluorescence. At these lower excitation densities, both measurements confirm that the initially excited singlet state relaxes with a decay time of 80 ± 3 ps, not 9.2 ps as claimed in the earlier paper. In order to investigate the origin of the singlet decay, the wavelength-resolved fluorescence dynamics were measured at 298 K, 77 K, and 4 K. A high-energy J-type emitting species undergo a rapid (100 ps) decay at all temperatures, while at 77 K and 4 K additional species with H-type and J-type emission lineshapes have much longer lifetimes. A global analysis of the wavelength-dependent decays shows that the initial ~100 ps decay occurs to a dark state and not via energy transfer to lower energy bright states. Varying the excitation wavelength from 400 nm to 510 nm had no effect on the fast decay, suggesting that there is no energy threshold for the initial singlet relaxation. The presence of different emitting species at different temperatures means that earlier interpretations of the fluorescence behavior in terms of one singlet state that is short-lived due to singlet fission at high temperatures but long-lived at lower temperatures are probably too simplistic. The presence of a rapid singlet decay at all temperatures indicates that the initially created J-type singlet exciton decays to an intermediate that only produces free triplets (and delayed fluorescence) at high temperatures.
多晶并四苯薄膜的激发态动力学研究采用飞秒瞬态吸收结合皮秒荧光,延续了早期论文[J. J. Burdett, A. M. Muller, D. Gosztola 和 C. J. Bardeen, J. Chem. Phys. 133, 144506 (2010)]中的工作。通过研究单线态衰减的强度依赖性,了解先前观察到的宽带瞬态吸收和荧光实验之间差异的起源。高灵敏度单通道瞬态吸收实验使我们能够将瞬态吸收动力学与在相同激光强度下测量的荧光动力学进行比较。在高激发密度下,激子-激子湮灭速率常数约为 1×10(-8) cm(3) s(-1),导致单线态快速衰减,但在激发密度为 2×10(17) cm(-3)或更低时,瞬态吸收的动力学与荧光的动力学相匹配。在这些较低的激发密度下,两种测量都证实初始激发的单线态以 80±3 ps 的衰减时间松弛,而不是早期论文中声称的 9.2 ps。为了研究单线态衰减的起源,在 298 K、77 K 和 4 K 下测量了波长分辨荧光动力学。在所有温度下,高能 J 型发射物种都经历快速(100 ps)衰减,而在 77 K 和 4 K 下,具有 H 型和 J 型发射线形状的其他物种具有更长的寿命。对波长相关衰减的全局分析表明,初始的100 ps 衰减发生到暗态,而不是通过能量转移到低能亮态。将激发波长从 400nm 变到 510nm 对快速衰减没有影响,这表明初始单线态弛豫没有能量阈值。不同温度下存在不同的发射物种意味着,以前基于高温下由于单线态裂变而导致短寿命的单态但在低温下长寿命的单态来解释荧光行为的解释可能过于简单。在所有温度下都存在快速的单线态衰减表明,最初形成的 J 型单线态激子衰减到一种中间体,该中间体仅在高温下产生游离三重态(和延迟荧光)。