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For the sake of complete explanation, some of the steady state absorption and photoluminescence data in Figure 1 and Table 1 were reproduced from our previous communication.
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For the sake of complete explanation, some of the steady state absorption and photoluminescence data in Figure 1 and Table 1 were reproduced from our previous communication.
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Although the ΔE (Eox, Ered) value does not exactly match phosphorescence energy of the corresponding Ir(III) complex, LUMO tuning with ancillary ligands can be evidenced by a linear proportionality between them
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red) value does not exactly match phosphorescence energy of the corresponding Ir(III) complex, LUMO tuning with ancillary ligands can be evidenced by a linear proportionality between them.
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See the Supporting Information for data of other Ir(III) complexes
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See the Supporting Information for data of other Ir(III) complexes.
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The early stage spectrum of 3 can be safely assigned as cyclometalating ligand-centered phosphorescence from the facts that (1) fluorescence from the free ancillary ligand (quinaldic acid)' was observed at 374 nm, thus eliminating contamination by fluorescence from the residual ancillary ligand (see the Supporting Information), and (2) all of 3 to 6, whose LUMOs exist in the ancillary ligands, showed early stage spectra with identical spectral position, excluding a possibility of singlet emission from Ir(III) complexes.
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The early stage spectrum of 3 can be safely assigned as cyclometalating ligand-centered phosphorescence from the facts that (1) fluorescence from the free ancillary ligand (quinaldic acid)' was observed at 374 nm, thus eliminating contamination by fluorescence from the residual ancillary ligand (see the Supporting Information), and (2) all of 3 to 6, whose LUMOs exist in the ancillary ligands, showed early stage spectra with identical spectral position, excluding a possibility of singlet emission from Ir(III) complexes.
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Instrument response function (IRF) was determined to be a Gaussian curve with a time constant of 13.04 ns. The decay fittings were made by using a least-squares deconvolution fitting process (LIFETIME program with an iterative nonlinear least-squares deconvolution procedure developed at the University of Pennsylvania, which ensures a temporal resolution of one third of IRF time constant. Practically, a time constant different from IRF time can be determined. In addition, our transient curves were averaged after accumulating thousands of times. We can find the difference in the initial rise of the prompt emission (C∧N) and the delayed emission (LX) of 3 in Figure 3d
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Instrument response function (IRF) was determined to be a Gaussian curve with a time constant of 13.04 ns. The decay fittings were made by using a least-squares deconvolution fitting process (LIFETIME program with an iterative nonlinear least-squares deconvolution procedure developed at the University of Pennsylvania), which ensures a temporal resolution of one third of IRF time constant. Practically, a time constant different from IRF time can be determined. In addition, our transient curves were averaged after accumulating thousands of times. We can find the difference in the initial rise of the prompt emission (C∧N) and the delayed emission (LX) of 3 in Figure 3d.
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ILET time scale of the ns regime can be rationalized by the fact that energy transfer takes place between spatially separated ligands cyclometalating dfppy and ancillary ligand
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ILET time scale of the ns regime can be rationalized by the fact that energy transfer takes place between spatially separated ligands (cyclometalating dfppy and ancillary ligand).
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ET = (τ - τ′)/τ, where.τ and τ′ denote the phosphorescence lifetime of 1 in the absence and presence of energy accepting red emitters, respectively.
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ET = (τ - τ′)/τ, where.τ and τ′ denote the phosphorescence lifetime of 1 in the absence and presence of energy accepting red emitters, respectively.
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