In the quest for coordination compounds with potential applications in energy conversion processes, a new series of four Ir(III) complexes (C1–4) of the type [Ir(R-ppy)2(Ln)](PF6), where R-ppy = 2-phenylpyridine (ppy) or 2,4-difluorophenylpyridine (F2-ppy) and Ln = 1-methyl-1H-pyrazole[30,40 :5,6]pyrazino[2,3-f]-[1,10]phenanthroline (L1) or thieno[30,40:5,6]pyrazino[2,3-f][1,10]phenanthroline (L2) has been synthesized. The photophysical properties of these compounds have been thoroughly characterized by both steadystate and time-resolved spectroscopic techniques, pointing out a complex interplay between excited states of different nature that plays a crucial role in the deactivation processes. In the case of complexes C1–2 that feature the same L1 ancillary ligand, the lowest excited states at room temperature are characterized by an admixture between the 3 MLCT/3 LLCT and 3 LC states, with an almost pure 3 LC character in C2. For C3–4, the admixture among charge-transfer and ligand-centred states is negligible, due to the appreciably low energy of the LC one, which, however, plays a non-innocent role in the deactivation pathway of the triplet charge-transfer emissive states of complexes C3–4. This work thus highlights the importance of a detailed comprehension of the photophysical properties of Ir(III) complexes in view of their use in energy transformation systems.

Substituent influence in phenanthroline-derived ancillary ligands on the excited state nature of novel cationic Ir(III) complexes

Mirco Natali
Secondo
;
2018

Abstract

In the quest for coordination compounds with potential applications in energy conversion processes, a new series of four Ir(III) complexes (C1–4) of the type [Ir(R-ppy)2(Ln)](PF6), where R-ppy = 2-phenylpyridine (ppy) or 2,4-difluorophenylpyridine (F2-ppy) and Ln = 1-methyl-1H-pyrazole[30,40 :5,6]pyrazino[2,3-f]-[1,10]phenanthroline (L1) or thieno[30,40:5,6]pyrazino[2,3-f][1,10]phenanthroline (L2) has been synthesized. The photophysical properties of these compounds have been thoroughly characterized by both steadystate and time-resolved spectroscopic techniques, pointing out a complex interplay between excited states of different nature that plays a crucial role in the deactivation processes. In the case of complexes C1–2 that feature the same L1 ancillary ligand, the lowest excited states at room temperature are characterized by an admixture between the 3 MLCT/3 LLCT and 3 LC states, with an almost pure 3 LC character in C2. For C3–4, the admixture among charge-transfer and ligand-centred states is negligible, due to the appreciably low energy of the LC one, which, however, plays a non-innocent role in the deactivation pathway of the triplet charge-transfer emissive states of complexes C3–4. This work thus highlights the importance of a detailed comprehension of the photophysical properties of Ir(III) complexes in view of their use in energy transformation systems.
2018
Gonzalez, Ivan; Natali, Mirco; Cabrera, Alan R.; Loeb, Barbara; Maze, Jeronimo; Dreyse, Paulina
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11392/2388481
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