Department of Chemistry and Center for Photochemical Sciences, Bowling Green State University, Bowling Green, Ohio 43403, USA.
J Am Chem Soc. 2010 Oct 13;132(40):14203-11. doi: 10.1021/ja105510k.
Selective near-IR (NIR) excitation (780 nm) of the conjugated supermolecule ruthenium(II) [15-(4'-ethynyl-(2,2';6',2''-terpyridinyl))-bis[(5,5',-10,20-di(2',6'-bis(3,3-dimethylbutoxy)phenyl)porphinato)zinc(II)]ethyne][4'-pyrrolidin-1-yl-2,2';6',2''-terpyridine] bis(hexafluorophosphate) (Pyr(1)RuPZn(2)) in solutions containing N,N-bis(ethylpropyl)perylene-3,4,9,10-tetracarboxylicdiimide (PDI) or tetracene gives rise to a substantial anti-Stokes energy gain (PDI, 0.70 eV; tetracene, 0.86 eV). Experimental data clearly demonstrate that this upconverted fluorescence signal is produced via Pyr(1)RuPZn(2)-sensitized triplet-triplet annihilation (TTA) photochemistry. The TTA process was confirmed by the quadratic dependence of the integrated (1)PDI* emission centered at 541 nm derived from 780 nm laser excitation. The T(1)→T(n) excited state absorption decay of Pyr(1)RuPZn(2), monitored at 900 nm as a function of PDI concentration, revealed Stern-Volmer and bimolecular quenching constants of 10 048 M(-1) and 5.9 × 10(8) M(-1) s(-1), respectively, for the PDI triplet sensitization process. The T(1)→T(n) PDI extinction coefficient at 560 nm (ε(T) = 6.6 × 10(4) M(-1) cm(-1)) was determined through the triplet energy transfer method utilizing anthracene as the donor chromophore. (3)PDI* transient triplet absorption dynamics observed as a function of 485 nm incident nanosecond pump laser fluence demonstrate a bimolecular (3)PDI*-(3)PDI* TTA rate constant (k(TT) = 1.0 ± 0.2 × 10(9) M(-1) s(-1)). The maximum quantum yield of the supermolecule-sensitized PDI upconverted emission (Φ(UC) = 0.0075 ± 0.0002) was determined relative to [Os(phen)(3)]PF(6) at an incident laser power of 22 mW at 780 nm. This study successfully demonstrates NIR-to-visible photon upconversion and achieves a new record anti-Stokes shift of 0.86 eV for sensitized TTA, using the supermolecular Pyr(1)RuPZn(2)sensitizer. The stability of the Pyr(1)RuPZn(2)/PDI chromophore combination is readily apparent as continuous irradiation at 780 nm produces 541 nm centered fluorescence with no significant decrease in intensity measured over time domains exceeding several hours. The molecular components of these NIR-to-vis upconverting compositions illustrate that substantial anti-Stokes energy gains via a TTA process can be effortlessly realized.
在含有 N,N-二(乙基丙基)苝-3,4,9,10-四羧酸二酰亚胺(PDI)或并四苯的溶液中,选择共轭超分子钌(II)[15-(4'-乙炔基-(2,2';6',2''-三联吡啶基))-双[(5,5',-10,20-二(2',6'-二(3,3-二甲基丁氧基)苯基)卟啉ato)锌(II)]乙炔][4'-吡咯烷-1-基-2,2';6',2''-三联吡啶]双(六氟磷酸盐)(Pyr(1)RuPZn(2))的近红外(NIR)(780nm)选择性激发会导致显著的反斯托克斯能量增益(PDI,0.70eV;并四苯,0.86eV)。实验数据清楚地表明,这种上转换荧光信号是通过 Pyr(1)RuPZn(2)敏化三重态-三重态湮灭(TTA)光化学反应产生的。TTA 过程通过从 780nm 激光激发衍生的中心位于 541nm 的集成(1)PDI发射的二次依赖性得到证实。Pyr(1)RuPZn(2)的 T(1)→T(n)激发态吸收衰减,作为 PDI 浓度的函数,在 900nm 处监测,分别为 PDI 三重态敏化过程的 Stern-Volmer 和双分子猝灭常数 10048M(-1)和 5.9×10(8)M(-1)s(-1)。通过利用蒽作为供体发色团的三重态能量转移方法,确定了 560nm 处的 T(1)→T(n)PDI 消光系数(ε(T)=6.6×10(4)M(-1)cm(-1))。作为 485nm 入射纳秒泵浦激光强度的函数观察到的(3)PDI瞬态三重态吸收动力学表明,双分子(3)PDI*-(3)PDITTA 速率常数(k(TT)=1.0±0.2×10(9)M(-1)s(-1))。相对于[Os(phen)(3)]PF(6),在 780nm 处的入射激光功率为 22mW 时,超分子敏化 PDI 上转换发射的最大量子产率(Φ(UC)=0.0075±0.0002)是通过(3)PDI的双分子(3)PDI*-(3)PDI*TTA 速率常数(k(TT)=1.0±0.2×10(9)M(-1)s(-1))确定的。该研究成功地证明了近红外到可见光子的上转换,并使用超分子 Pyr(1)RuPZn(2)敏化剂实现了新的记录为 0.86eV 的敏化 TTA 反斯托克斯位移。Pyr(1)RuPZn(2)/PDI 发色团组合的稳定性很明显,因为在 780nm 处连续照射会产生以 541nm 为中心的荧光,在超过几个小时的时间范围内,强度没有明显下降。这些近红外到可见上转换组合物的分子组成表明,可以轻松地实现通过 TTA 过程的实质性反斯托克斯能量增益。