“…Figure 7d). Listed below were selective Os(II), Ir(III), and Pt(II) based NIR emitters showing emission peak wavelength at ∼700 nm: CNIr (𝜆 max = 690 nm, EQE max = 2.75%), [41] Ir(dpa-piq-CN) 2 (acac) (𝜆 max = 692 nm, EQE max = 12.5%), [42] Ir(ttiq) 2 (tmd) (𝜆 max = 696 nm, EQE max = 13.7%), [43] (o-CF 3 piq) 2 Ir(dipg) (𝜆 max = 704 nm, EQE max = 4.6%), [44] Ir3 (𝜆 max = 708 nm, EQE max = 13.7%), [45] ( t BuTPA-DBPz) 2 Ir(acac) (𝜆 max = 714 nm, EQE max = 12.3%), [46] Ir4 (𝜆 max = 714 nm, EQE max = 1.08%), [47] (PPz-11,12-DO) 2 Ir(acac) (𝜆 max = 724 nm, EQE max = 4.14%), [48] 2 (𝜆 max = 760 nm, EQE max = 4.5%), [49] TPAIr (𝜆 max = 768 nm, EQE max = 3.34%), [10e] Ir(mpbqx-g) 2 (acac) (𝜆 max = 780 nm, EQE max = 2.2%), [50] 3 (𝜆 max = 725 nm, EQE max = 2.2%), [51] Pt-3 (𝜆 max = 740 nm, EQE max = 10.8%), [ 16a ] D3 (𝜆 max = 754 nm, EQE max = 3.0%), [ 16b ] (BOiqn) 2 Pt (𝜆 max = 656 nm, EQE max = 3.8%), [ 16c ] and tz2 (𝜆 max = 746 nm, EQE max = 4.2%). [ 9a ] It is also worth noting that both the structureless emission profile and low efficiency roll-offs are observed at high current densities with our bis-tridentate Ir(III) emitters.…”