We present an experimental and theoretical study of aggregate excited states formed by complexes of the type Pt(N^C^N)Cl, which display near-infrared (NIR) photoluminescence in film and NIR electroluminescence in OLED...
The ancillary ligand X strongly influences the aggregates formed by complexes of the type Pt(N^C^N)X. X = I leads to a 4× increase in film PLQY and OLED EQE vs. X = Cl, while X = SCN yields very long wavelength electroluminescence, λmaxEL = 944 nm.
We report a combined experimental and theoretical study of a series of thiomethyl (SMe) anchored cross-conjugated molecules featuring an acyclic central bridging ketone and their analogous skipped-conjugated alcohol derivatives. Studies of these molecules in a gold|single-molecule|gold junction using scanning tunneling microscopy-break junction techniques reveal a similar conductance (G) value for both the cross-conjugated molecules and their skipped-conjugated partners. Theoretical studies based on density functional theory of the molecules in their optimum geometries in the junction reveal the reason for this similarity in conductance, as the predicted conductance for the alcohol series of compounds varies more with the tilt angle. Thermopower measurements reveal a higher Seebeck coefficient (S) for the cross-conjugated ketone molecules relative to the alcohol derivatives, with a particularly high S for the biphenyl derivative 3a (−15.6 μV/K), an increase of threefold compared to its alcohol analog. The predicted behavior of the quantum interference (QI) in this series of cross-conjugated molecules is found to be constructive, though the appearance of a destructive QI feature for 3a is due to the degeneracy of the HOMO orbital and may explain the enhancement of the value of S for this molecule.
A series of seven new platinum(II) complexes PtL
n
Cl have been prepared, where L
n
is an NCN-coordinating ligand comprising
a benzene
ring 1,3-disubstituted with two different azaheterocycles. In PtL1–5Cl, one heterocycle is a simple pyridine ring, while
the other is an isoquinoline, a quinoline, a pyrimidine (L1, L2, L3), or a p-CF3- or p-OMe-substituted pyridine (L4 and
L5). PtL6Cl incorporates both a p-CF3 and a p-OMe-substituted pyridine.
The synthesis of the requisite proligands HL
n
is achieved using Pd-catalyzed cross-coupling methodology.
The molecular structures of six of the Pt(II) complexes have been
determined by X-ray diffraction. All the complexes are brightly luminescent
in deoxygenated solution at room temperature. The absorption and emission
properties are compared with those of the corresponding symmetrical
complexes featuring two identical heterocycles, PtL
nsymCl, and of the parent Pt(dpyb)Cl containing two unsubstituted
pyridines [dpybH = 1,3-di(2-pyridyl)benzene]. While the absorption
spectra of the nonsymmetrical complexes show features of both PtL
nsymCl and Pt(dpyb)Cl, the emission generally
resembles that of whichever of the corresponding symmetrical complexes
has the lower-energy emission. PtL1Cl differs in thatat
room temperature but not at 77 Kit displays emission bands
that can be attributed to excited states involving both the pyridine
and the isoquinoline rings, despite the latter being unequivocally
lower in energy. This unusual behavior is attributed to thermally
activated repopulation of the former excited state from the latter,
facilitated by the very long-lived nature of the isoquinoline-based
excited state. At elevated concentrations, all the complexes show
an additional red-shifted emission band attributable to excimers.
For PtL1Cl, the excimer strikingly dominates the emission
spectra at all but the lowest concentrations (<10–5 M). Trends in the energies of the excimers and their propensity
to form are compared with those of the symmetrical analogues.
We present a study of aggregate excited states formed by complexes of the type Pt(N^C^N)X, where N^C^N represents a tridentate cyclometallating ligand, and X = SCN or I. These materials display near-infrared (NIR) photoluminescence in film and electroluminescence in NIR OLEDs with λELmax = 720-944 nm. We demonstrate that the two monodentate ligands X employed modulate aggregate formation compared to the parent complexes where X = Cl. While the identity of the monodentate ligand affects the energy of Pt–Pt excimers in solution in only a subtle way, it strongly influences aggregation in film. Detailed calculations on aggregates of different sizes support the experimental conclusions from steady-state and time-resolved luminescence studies at variable temperatures. The use of X = I appears to limit aggregation to the formation of dimers, while X = SCN promotes the formation of larger aggregates, such as tetramers and pentamers, leading in turn to NIR photo- and electroluminescence > 850 nm. A possible explanation for the contrasting influence of the monodentate ligands is the lesser steric hindrance associated with the SCN group compared to the bulkier I ligand. By exploiting the propensity of the SCN complexes to form extended aggregates, we have prepared an NIR-emitting OLED that shows very long-wavelength electroluminescence, with λEL(max) = 944 nm and a maximum EQE = 0.3 ± 0.1 %. Such data appear to be unprecedented for a device relying on a Pt(II) complex aggregate as the emitter.
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