19 research outputs found
Electroluminescence Stability of Organic Light-Emitting Devices Utilizing a Nondoped Pt-Based Emission Layer
We
study the effects of using an emitting material (PtÂ(II) bisÂ(3-(trifluoromethyl)-5-(2-pyridyl)Âpyrazolateî—¸PtÂ(fppz)<sub>2</sub>) characterized by a preferred horizontal dipole alignment
and a nearly unitary quantum yield regardless of concentration on
the lifetime of organic light-emitting devices (OLEDs). Using such
a material as a dopant in increasingly higher concentrations is found
to lead to an increase in device stability, a trend that is different
from that commonly observed with conventional OLED guests. The results
are consistent with the newly discovered exciton–polaron-induced
aggregation degradation mechanism of OLED materials. When this emitter
is used as a neat emission layer, the material is already in a highly
aggregated state, and the device is no longer affected by exciton–polaron
interactions. The results demonstrate the potential stability benefits
of using such materials in OLEDs
Phosphorescent PtAu<sub>2</sub> Complexes with Differently Positioned Carbazole–Acetylide Ligands for Solution-Processed Organic Light-Emitting Diodes with External Quantum Efficiencies of over 20%
The utilization of
phosphorescent metal cluster complexes as new
types of emitting materials in organic light-emitting diodes (OLEDs)
is becoming an alternative and viable approach for achieving high-efficiency
electroluminescence. We report herein the design of cationic PtAu<sub>2</sub> cluster complexes with differently positioned 9-phenylcarbazole–acetylides
to serve as phosphorescent emitters in OLEDs. The rigid structures
of PtAu<sub>2</sub> complexes cause intense phosphorescence with quantum
yields of over 85%, which originates from <sup>3</sup>[Ď€Â(phenylcarbazole–acetylide)
→ Ď€*Â(dpmp)] ligand-to-ligand and <sup>3</sup>[Ď€Â(phenylcarbazole–acetylide)
→ p/sÂ(PtAu<sub>2</sub>)] ligand-to-metal charge-transfer triplet
excited states. When 8 wt % PtAu<sub>2</sub> is doped to blended host
materials of TCTA and OXD-7 (2:1 weight ratio) as light-emitting layers,
solution-processed OLEDs give a current efficiency of 78.2 cd A<sup>–1</sup> and an external quantum efficiency (EQE) of 21.5%
at a practical luminance of 1029 cd m<sup>–2</sup> with a slow
efficiency roll-off upon increasing luminance. This represents the
best device performance and the highest efficiency recorded at practical
luminance for solution-processed OLEDs
Bis-tridentate Ir(III) Phosphors and Blue Hyperphosphorescence with Suppressed Efficiency Roll-Off at High Brightness
Narrowband blue emitters are indispensable in achieving
ultrahigh-definition
OLED displays that satisfy the stringent BT 2020 standard. Hereby,
a series of bis-tridentate Ir(III) complexes bearing electron-deficient
imidazo[4,5-b]pyridin-2-ylidene carbene coordination
fragments and 2,6-diaryloxy pyridine ancillary groups were designed
and synthesized. They exhibited deep blue emission with quantum yields
of up to 89% and a radiative lifetime of 0.71 ÎĽs in the DPEPO
host matrix, indicating both the high efficiency and excellent energy
transfer process from the host to dopant. The OLED based on Irtb1 showed an emission at 468 nm with a maximum external
quantum efficiency (EQE) of 22.7%. Moreover, the hyper-OLED with Irtb1 as a sensitizer for transferring energy to terminal
emitter v-DABNA exhibited a narrowband blue emission at 472 nm and
full width at half-maximum (FWHM) of 24 nm, a maximum EQE of 23.5%,
and EQEs of 19.7, 16.1, and 12.9% at a practical brightness of 100,
1000, and 5000 cd/m2, respectively
Theoretical Study of N749 Dyes Anchoring on the (TiO<sub>2</sub>)<sub>28</sub> Surface in DSSCs and Their Electronic Absorption Properties
We have performed calculations on the panchromatic N749
dyes adsorbed on the (TiO<sub>2</sub>)<sub>28</sub> surface. N749
is a prototypical form of RuÂ(II) complexes for dye sensitized solar
cells (DSSCs), which possesses a terpyridine tridentate ligand bearing
four different protonation states (0, 1, 2, or 3 carboxylic protons).
Depending on the type of proton bonding interaction (protonated and
deprotonated), seven N749/(TiO<sub>2</sub>)<sub>28</sub> surface models
(N749-0H/(TiO<sub>2</sub>)<sub>28</sub>, N749-1H-P/(TiO<sub>2</sub>)<sub>28</sub>, N749-1H-DP/(TiO<sub>2</sub>)<sub>28</sub>, N749-2H-P/(TiO<sub>2</sub>)<sub>28</sub>, N749-2H-DP/(TiO<sub>2</sub>)<sub>28</sub>,
N749-3H-P/(TiO<sub>2</sub>)<sub>28</sub>, and N749-3H-DP/(TiO<sub>2</sub>)<sub>28</sub>) have been applied in this study for the geometry
optimization, frontier molecular orbital level diagrams, and calculated
absorption spectra. The moderate surface area of the (TiO<sub>2</sub>)<sub>28</sub> cluster is suitable for N749 dyes adsorbing behaviors
so that all calculations can be performed using the Gaussian 09 program
package. We have carefully examined these seven N749/(TiO<sub>2</sub>)<sub>28</sub> assemblies that could influence the DSSC device performance.
The calculated absorption spectra of these seven various N749/(TiO<sub>2</sub>)<sub>28</sub> models are in good agreement with the experimental
results by Hagfeldt et al. (<i>J</i>. <i>Phys</i>. <i>Chem</i>. <i>B</i> <b>2002</b>, <i>106</i>, 12693–12704) with onset ranging from the visible
to near-IR region. The combination of the adsorption energy onto TiO<sub>2</sub> and calculated absorption spectra (cf. the experimental results)
concludes that the deprotonated dyes constitute the most favorable
and dominant structure in the DSSC devices. The frontier molecular
orbital graphs indicate that the electron charge distributions of
all HOMOs are located at the N749 dyes, while LUMOs are localized
at the (TiO<sub>2</sub>)<sub>28</sub> surface or delocalized at the
interfacial regions of N749/(TiO<sub>2</sub>)<sub>28</sub>. The corresponding
transitions are thus more like a type of optical electron transfer,
injecting the electron to the interfacial TiO<sub>2</sub>
Iridium(III) Complexes Bearing Tridentate Chromophoric Chelate: Phosphorescence Fine-Tuned by Phosphine and Hydride Ancillary
Functional 2-pyrazolyl-6-phenylpyridine
chelatesî—¸namely, (pzpyph<sup>Bu</sup>)ÂH<sub>2</sub> and (pzpyph<sup>CF<sub>3</sub></sup>)ÂH<sub>2</sub> and phosphinesî—¸are successfully
employed in the preparation of emissive IrÂ(III) metal complexes, for
which the reaction with phosphine such as PPh<sub>3</sub>, PPh<sub>2</sub>Me, and PPh<sub>2</sub>(CH<sub>2</sub>Ph) afford corresponding
IrÂ(III) complexes [IrÂ(pzpyph<sup>Bu</sup>)Â(PPh<sub>3</sub>)<sub>2</sub>H] (<b>1a</b>), [IrÂ(pzpyph<sup>CF<sub>3</sub></sup>)Â(PPh<sub>2</sub>R)<sub>2</sub>H] (<b>2a</b>–<b>2c</b>),
R = Ph, Me, CH<sub>2</sub>Ph, which also show an equatorial coordinated
hydride. In contrast, treatment with 1,2-bisÂ(diphenylphosphino)Âbenzene
(dppb) and 1,2-bisÂ(diphenylphosphino)Âethane (dppe) yields the isomeric
products [IrÂ(pzpyph<sup>Bu</sup>)Â(dppb)ÂH] (<b>3a</b>) and [IrÂ(pzpyph<sup>Bu</sup>)Â(dppe)ÂH] (<b>3b</b>), for which the distinctive, axial
hydride undergoes rapid chlorination, forming chlorinated complexes
[IrÂ(pzpyph<sup>Bu</sup>)Â(dppb)ÂCl] (<b>4a</b>) and [IrÂ(pzpyph<sup>Bu</sup>)Â(dppe)ÂCl] (<b>4b</b>), respectively. On the other
hand, upon extensive heating of <b>2c</b>, one of its coordinated
PPh<sub>2</sub>(CH<sub>2</sub>Ph) exhibits benzyl cyclometalation
and hydride elimination to afford [IrÂ(pzpyph<sup>CF<sub>3</sub></sup>)Â(PPh<sub>2</sub>R)Â(PPh<sub>2</sub>R′)] (<b>5c</b> and <b>6c</b>) R = CH<sub>2</sub>Ph and R′ = CH<sub>2</sub>(<i>o</i>-C<sub>6</sub>H<sub>4</sub>) as the kinetic and thermodynamic
products, respectively. Their
structural, photophysical, and electrochemical properties are examined
and further affirmed by the computational approaches
Harvesting Highly Electronically Excited Energy to Triplet Manifolds: State-Dependent Intersystem Crossing Rate in Os(II) and Ag(I) Complexes
A series of newly synthesized OsÂ(II) and AgÂ(I) complexes
exhibit
remarkable ratiometric changes of intensity for phosphorescence versus
fluorescence that are excitation wavelength dependent. This phenomenon
is in stark contrast to what is commonly observed in condensed phase
photophysics. While the singlet to triplet intersystem crossing (ISC)
for the titled complexes is anomalously slow, approaching several
hundred picoseconds in the lowest electronic excited state (S<sub>1</sub> → T<sub>1</sub>), higher electronic excitation leads
to a much accelerated rate of ISC (10<sup>11</sup>–10<sup>12</sup> s<sup>–1</sup>), which is competitive with internal conversion
and/or vibrational relaxation, as commonly observed in heavy transition
metal complexes. The mechanism is rationalized by negligible metal
d orbital contribution in the S<sub>1</sub> state for the titled complexes.
Conversely, significant ligand-to-metal charge transfer character
in higher-lying excited states greatly enhances spin–orbit
coupling and hence the ISC rate. The net result is to harvest high
electronically excited energy toward triplet states, enhancing the
phosphorescence
Mechanistic Investigation of Improved Syntheses of Iridium(III)-Based OLED Phosphors
Treatment of [IrCl<sub>3</sub>(tht)<sub>3</sub>] (tht
= tetrahydrothiophene)
with a stoichiometric amount of PPh<sub>3</sub> gave the monosubstitution
product [IrÂ(tht)<sub>2</sub>(PPh<sub>3</sub>)ÂCl<sub>3</sub>] (<b>5</b>), whose synthesis, particularly that leading to the effective
preparation of OLED phosphors, was studied and optimized to achieve
the best product yields. Thus, the independent treatment of <b>5</b> with 2,4-difluorophenylpyridine (dfppyH) or with variable
amounts of benzyldiphenylphosphine (bdpH) gave rise to the formation
of the cyclometalation products [IrÂ(dfppy)Â(tht)Â(PPh<sub>3</sub>)ÂCl<sub>2</sub>] (<b>7</b>), [IrÂ(bdp)Â(bdpH)Â(tht)ÂCl<sub>2</sub>] (<b>8</b>), and [IrÂ(bdp)Â(PPh<sub>3</sub>)Â(tht)ÂCl<sub>2</sub>] (<b>10</b>), depending on the stoichiometry and conditions employed.
Upon further treatment with 5-pyridyl-3-trifluoromethyl-1<i>H</i>-pyrazole (fppzH), these IrÂ(III) complexes <b>7</b>, <b>8</b>, and <b>10</b> were capable of yielding the phosphors
[IrÂ(dfppy)Â(fppz)<sub>2</sub>] (<b>1</b>), [IrÂ(bdp)<sub>2</sub>(fppz)] (<b>4</b>), and [IrÂ(bdp)Â(fppz)<sub>2</sub>] (<b>2</b>), respectively. The general mechanism en route to their
formation was studied and discussed
Sky Blue-Emitting Iridium(III) Complexes Bearing Nonplanar Tetradentate Chromophore and Bidentate Ancillary
Tetradentate chelates
bearing tripodal arranged terpyridine and a functional pyrazole unit
(i.e., L1-H and L2-H) were employed in preparation of IrÂ(III) complexes
[IrÂ(L1)ÂCl<sub>2</sub>] (<b>1</b>) and [IrÂ(L2)ÂCl<sub>2</sub>]
(<b>2</b>); subsequent chloride-to-bipyrazolate substitution
gave [IrÂ(L1)Â(bipz)] (<b>3</b>) and [IrÂ(L2)Â(bipz)] (<b>4</b>). Single-crystal X-ray structural studies on <b>1</b> and <b>3</b> showed the possession of a tetradentate chelate, whereas
the remaining <i>cis</i>-sites are occupied by either dual
chlorides or the bipz chelate, respectively. Sky blue organic light-emitting
diode with peak efficiencies (10.1%, 19.8 cd·A<sup>–1</sup>, and 20.4 lm·W<sup>–1</sup>) was successfully fabricated
using <b>3</b> (or <b>4</b>) as dopant emitter, highlighting
the potential application of this class of IrÂ(III) phosphor
4,4′,5,5′-Tetracarboxy-2,2′-bipyridine Ru(II) Sensitizers for Dye-Sensitized Solar Cells
Two RuÂ(II) sensitizers TCR-1 and
TCR-2 bearing four carboxy anchoring groups were prepared using 4,4′,5,5′-tetraethoxycarbonyl-2,2′-bipyridine
chelate and 4-(5-hexylthien-2-yl)-2-(3-trifluoromethyl-1<i>H</i>-pyrazol-5-yl)Âpyridine and 6-<i>t</i>-butyl-1-(3-trifluoromethyl-1<i>H</i>-pyrazol-5-yl)Âisoquinoline, respectively. Dissolution
of these sensitizers in DMF solution afforded a light green solution
up to 10<sup>–5</sup> M, for which their color gradually turned
red upon further dilution and deposition on the surface of a TiO<sub>2</sub> photoanode due to the spontaneous deprotonation of carboxylic
acid groups. These sensitizers were characterized using electrochemical
means and structural analysis time-dependent density functional theory
(TDDFT) simulation and were also subjected to actual device fabrication.
The as-fabricated DSC devices showed overall efficiencies η
= 6.16% and 6.23% versus their 4,4′-dicarboxy counterparts
TFRS-2 and TFRS-52 with higher efficiencies of 7.57% and 8.09%, using
electrolyte with 0.2 M LiI additive. Their inferior efficiencies are
possibly caused by the combination of blue-shifted absorption on TiO<sub>2</sub>, inadequate dye loading, and the perpendicularly oriented
central carboxy groups
The Empirical Correlation between Hydrogen Bonding Strength and Excited-State Intramolecular Proton Transfer in 2-Pyridyl Pyrazoles
A series of 2-pyridyl pyrazoles <b>1a</b> and <b>1</b>–<b>5</b> with various functional groups attached
to
either pyrazole or pyridyl moieties have been strategically designed
and synthesized in an aim to probe the hydrogen bonding strength in
the ground state versus dynamics of excited-state intramolecular proton
transfer (ESIPT) reaction. The title compounds all possess a five-membered-ring
(pyrazole)ÂN–H···NÂ(pyridine) intramolecular hydrogen
bond, in which both the N–H bond and the electron density distribution
of the pyridyl nitrogen lone-pair electrons are rather directional,
so that the hydrogen bonding strength is relatively weak, which is
sensitive to the perturbation of subtle chemical substitution and
consequently reflected from the associated ESIPT dynamics. Various
approaches such as <sup>1</sup>H NMR (N–H proton) to probe
the hydrogen bonding strength and absorption titration to assess the
acidity-basicity property were made for all the title analogues. The
results, together with supplementary support provided by a computational
approach, affirm that the increase of acidity (basicity) on the hydrogen
bonding donor (acceptor) sites leads to an increase of hydrogen-bonding
strength among the title 2-pyridyl pyrazoles. Luminescence results
and the associated ESIPT dynamics further reveal an empirical correlation
in that the increase of the hydrogen bonding strength leads to an
increase of the rate of ESIPT for the title 2-pyridyl pyrazoles, demonstrating
an interesting relationship among N–H acidity, hydrogen bonding
strength, and the associated ESIPT rate