Four cationic iridium
complexes
with 5-phenyl-1H-1,2,4-triazole (phtz) type cyclometalating
ligands (C^N) and different
ancillary ligands (N^N), namely, [Ir(dphtz)2(bpy)]PF6 (1), [Ir(dphtz)2(pzpy)]PF6 (2), [Ir(Mephtz)2(pzpy)]PF6 (3), and [Ir(Mephtz)2(dma-pzpy)]PF6 (4), have been designed, synthesized, and fully characterized
(dphtz = 1-(2,6-dimethylphenyl)-3-methyl-5-phenyl-1H-1,2,4-triazole, Mephtz = 1,3-dimethyl-5-phenyl-1H-1,2,4-triazole; bpy = 2,2′-bipyridine, pzpy = 2-(1H-pyrazol-1-yl)pyridine, dma-pzpy = 4-dimethylamino-2-(1H-pyrazol-1-yl) pyridine). In solution, complex 1 emits efficient yellow light (λmax = 547 nm), which
is blue-shifted by nearly 40 nm (or by 1187 cm–1) compared with that from the archetypal complex [Ir(ppy)2(bpy)]PF6 (Hppy = 2-phenylpyridine), owing to the stabilization
of the highest occupied molecular orbital by the phtz-type C^N ligand.
In the lightly doped rigid films, complex 1 emits green
light with a high luminescent efficiency of 0.89. Although complexes 2–4 with electron-rich N^N ligands are
weakly emissive or nearly nonemissive in the solution, they emit relatively
strong deep-blue light peaked around 435 and 461 nm in the lightly
doped films, which is among the bluest reported for cationic iridium
complexes. Theoretical calculations reveal that for complex 1, the emission always comes from the charge-transfer (CT)
(Ir/C^N → N^N) state; for complexes 2 and 3, the 3CT and C^N-centered 3π–π*
states lie close in energy and the emission could originate from either
or both of them; for complex 4, the emission comes predominantly
from the C^N-centered 3π–π* state. For
blue-emitting complexes 2–4, metal-centered
states play an active role in the nonradiative deactivation of the
emitting triplet states. Solid-state light-emitting electrochemical
cells (LECs) based on complexes 1–3 show yellow-green, blue, and blue-green electroluminescence, respectively,
with the yellow-green LEC affording a peak current efficiency of 21.5
cd A–1.