2013
DOI: 10.1016/j.jorganchem.2013.04.009
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Synthesis, structure, and solid-state phosphorescence of heteroleptic platinum(II) complexes bearing iminophenyl and iminophenoxy ligands

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Cited by 12 publications
(6 citation statements)
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“…Compounds 3g , h , which contain a methoxy group at the 2-position together with fluoro substituents at the 3- and 4-positions, also display a small red shift in comparison with the unsubstituted analogues 3e , f . Similar effects in the emission wavelengths due to the presence of fluoro or methoxy substituents have been previously reported. , …”
Section: Resultssupporting
confidence: 87%
“…Compounds 3g , h , which contain a methoxy group at the 2-position together with fluoro substituents at the 3- and 4-positions, also display a small red shift in comparison with the unsubstituted analogues 3e , f . Similar effects in the emission wavelengths due to the presence of fluoro or methoxy substituents have been previously reported. , …”
Section: Resultssupporting
confidence: 87%
“…The platinum satellites for the imine resonances (JHPt ~ 62 Hz) are consistent with other (salicylaldiminato)platinum complexes [18][19][20][21][22][23][24][25][26]. The FT-IR spectra show the expected decrease in the frequency of the C=N bond due to complexation, which is observed as the νC=N stretch shifts from ca.1632 cm -1 for the free ligands to ca.…”
supporting
confidence: 82%
“…This is a clear indication that consecutive π‐stacking interaction strongly diminishes efficient phosphorescent emission, while the herringbone motif caused by CH–π interactions and “isolated” stacking dimers does not have a negative influence on the solid‐state emission. The beneficial feature of CH–π interactions in solid‐state emission has also been observed in the high quantum efficiencies and heat‐resistance properties of heteroleptic platinum(II) complexes bearing iminophenyl and iminophenoxy ligands 14. The amorphous solid 1 e has less ordered molecular aggregation in which coordination planes are randomly dispersed, as shown in Figure 10 c.…”
Section: Resultsmentioning
confidence: 88%
“…The low heatresistance properties of these crystals (1 d: F 298K/ F 77K = 0.31; 1 e: F 298K/ F 77K = 0.26; 1 f: F 298K/ F 77K = 0.12) are attributable to weak molecular constraints within the crystals, in which each molecular unit is poorly bound with 1D regional offset stacking and van der Waals interactions. [14] The amorphous solid 1 e has less ordered molecular aggregation in which coordination planes are randomly dispersed, as shown in Figure 10 c. The quantum efficiency of amorphous 1 e at 77 K (F 77K = 0.22) is much higher than that of thermodynamic crystals of 1 e (F 77K = 0.08), which can be ascribed to the inhibition of energy dispersion by molecular alignment with less stacking. Thus, the "isolated" form of the p-stacking dimer formed inside the crystal lattice ( Figure 8 d and 9d) does not significantly affect the inhibition of solidstate emission.…”
Section: C1a C H T U N G T R E N N U N G (Unit A)) and 285 (H6amentioning
confidence: 96%
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