Bifurcation of Excited-State Population Leads to Anti-Kasha Luminescence in a Disulfide-Decorated Organometallic Rhenium Photosensitizer
J. E. FRANZ, Manuel Oelschlegel, J. Patrick Zobel, Shao‐An Hua, Jan-Hendrik Borter, Lucius Schmid, Giacomo Morselli, Oliver S. Wenger, Dirk Schwarzer, Franc Meyer, Leticia González
Abstract
High Resolution Image Download MS PowerPoint Slide We report a rhenium diimine photosensitizer equipped with a peripheral disulfide unit on one of the bipyridine ligands, [Re(CO) 3 (bpy)( S–S bpy 4,4 )] + ( 1 +, bpy = 2,2′-bipyridine, S–S bpy 4,4 = [1,2]dithiino[3,4- c:6,5- c ′]dipyridine), showing anti-Kasha luminescence. Steady-state and ultrafast time-resolved spectroscopies complemented by nonadiabatic dynamics simulations are used to disclose its excited-state dynamics. The calculations show that after intersystem crossing the complex evolves to two different triplet minima: a ( S–S bpy 4,4 )-ligand-centered excited state ( 3 LC) lying at lower energy and a metal-to-(bpy)-ligand charge transfer ( 3 MLCT) state at higher energy, with relative yields of 90% and 10%, respectively. The 3 LC state involves local excitation of the disulfide group into the antibonding σ* orbital, leading to significant elongation of the S–S bond. Intriguingly, it is the higher-lying 3 MLCT state, which is assigned to display luminescence with a lifetime of 270 ns: a signature of anti-Kasha behavior. This assignment is consistent with an energy barrier ≥ 0.6 eV or negligible electronic coupling, preventing reaction toward the 3 LC state after the population is trapped in the 3 MLCT state. This study represents a striking example on how elusive excited-state dynamics of transition-metal photosensitizers can be deciphered by synergistic experiments and state-of-the-art calculations. Disulfide functionalization lays the foundation of a new design strategy toward harnessing excess energy in a system for possible bimolecular electron or energy transfer reactivity.