The influence of thiolate ligands on the luminescence properties of cycloplatinated(ii) complexes.

Complexes [Pt(C^ N)(PPh3 )Cl] (C^ N = bzq (7,8-benzoquinolinyl, A) and ppy (2-phenylpyridinyl, B)) were reacted with various thiolate ligands to afford complexes [Pt(C^ N)(PPh3 )(κ1 -S-SR)], C^ N = bzq, R = SPh (thiophenolate, 1a); C^ N = ppy, R = SPh (1b); C^ N = bzq, R = Spy (pyridine-2-thiolate, 2a); C^ N = ppy, R = Spy (2b); C^ N = bzq, R = SpyN (pyrimidine-2-thiolate, 3a); C^ N = ppy, R = SpyN (3b). Complexes 1-3 were characterized by NMR spectroscopy, and the solid-state structures of 1a and 2a were determined by X-ray diffraction methods. Replacing a chloride ligand with electron-rich thiolates changes the lowest energy singlet and triplet excited states to the ones that feature charge transfer from the thiolate (mixed with some metal character) to the C^ N ligand, which was supported by TD-DFT calculations. All complexes are emissive at 298 K in the solid state except 2b and 3b, which are emissive only at 77 K having a less rigid structure compared to others. The emission of 1a and 1b originates from a low-energy excited state of dPt /πSR → π*C^N while 3a exhibits a3 LC/3 MLCT transition. For 1a and 1b, the radiative rate and the quantum efficiency are higher in a rigid environment such as a solid compared to a polymer and solution. Decreasing the rigidity of the environment leads to a flexibility of rotation of the -SR around the axis of the Pt-S bond. So the geometry can be easily changed after radiation and the lowest lying triplet excited state would have the effective contribution of the dd* transition, which opens a nonradiative pathway at room temperature.