35 research outputs found
Gram Scale Synthesis of Benzophenanthroline and Its Blue Phosphorescent Platinum Complex
The
design, synthesis, and characterization of 12-phenylÂbenzoÂ[<i>f</i>]Â[1,7]Âphenanthroline, Bzp, is reported. Its
use as a fluorine-free ligand for sky blue phosphorescence is demonstrated
in a cyclometalated platinum complex, BzpPtDpm. BzpPtDpm phosphoresces
at the same wavelength as its analogous 4,6-difluoroÂphenylÂpyridine
complex at both room temperature (466 nm) and 77 K (458 nm). Finally,
production of a conformationally restricted derivative of BzpPtDpm
with greatly increased quantum yield (46%) validates the versatility
of the synthetic route
Cu<sub>4</sub>I<sub>4</sub> Clusters Supported by P<sup>â§</sup>N-type Ligands: New Structures with Tunable Emission Colors
A series of Cu<sub>4</sub>I<sub>4</sub> clusters (<b>1</b>â<b>5</b>) supported by two P<sup>â§</sup>N-type
ligands 2-[(di<b>R</b>phosphino)Âmethyl]Âpyridine (<b>1</b>, R = phenyl; <b>2</b>, R = cyclohexyl; <b>3</b>, R = <i>tert</i>-butyl; <b>4</b>, R = <i>iso</i>-propyl; <b>5</b>, R = ethyl) have been synthesized. Single crystal X-ray
analyses show that all five clusters adopt a rare âoctahedralâ
geometry. The central core of the cluster consists of the copper atoms
arranged in a parallelogram with Ό<sup>4</sup>-iodides above
and below the copper plane. The copper atoms on the two short edges
of the parallelogram (CuâCu = 2.525(2)â2.630(1) Ă
)
are bridged with Ό<sup>2</sup>-iodides, whereas the long edges
(CuâCu = 2.839(3)â3.035(2) Ă
) are bridged in an
antiparallel fashion by the P<sup>â§</sup>N ligands. This Cu<sub>4</sub>I<sub>4</sub> geometry differs significantly from the âcubaneâ
and âstairstepâ geometries reported for other Cu<sub>4</sub>I<sub>4</sub>L<sub>4</sub> clusters. Luminescence spectra
of clusters <b>3</b> and <b>4</b> display a single emission
around 460 nm at room temperature that is assigned to emission from
a triplet halide-to-ligand charge-transfer (<sup>3</sup>XLCT) excited
state, whereas clusters <b>1</b>, <b>2</b>, and <b>5</b> also have a second band around 570 nm that is assigned to
a Cu<sub>4</sub>I<sub>4</sub> cluster-centered (<sup>3</sup>CC) excited
state. The structural and photophysical properties of a dinuclear
Cu<sub>2</sub>I<sub>2</sub>(P<sup>â§</sup>N)<sub>2</sub> complex
obtained during the sublimation of cluster <b>3</b> is also
provided
Cu<sub>4</sub>I<sub>4</sub> Clusters Supported by P<sup>â§</sup>N-type Ligands: New Structures with Tunable Emission Colors
A series of Cu<sub>4</sub>I<sub>4</sub> clusters (<b>1</b>â<b>5</b>) supported by two P<sup>â§</sup>N-type
ligands 2-[(di<b>R</b>phosphino)Âmethyl]Âpyridine (<b>1</b>, R = phenyl; <b>2</b>, R = cyclohexyl; <b>3</b>, R = <i>tert</i>-butyl; <b>4</b>, R = <i>iso</i>-propyl; <b>5</b>, R = ethyl) have been synthesized. Single crystal X-ray
analyses show that all five clusters adopt a rare âoctahedralâ
geometry. The central core of the cluster consists of the copper atoms
arranged in a parallelogram with Ό<sup>4</sup>-iodides above
and below the copper plane. The copper atoms on the two short edges
of the parallelogram (CuâCu = 2.525(2)â2.630(1) Ă
)
are bridged with Ό<sup>2</sup>-iodides, whereas the long edges
(CuâCu = 2.839(3)â3.035(2) Ă
) are bridged in an
antiparallel fashion by the P<sup>â§</sup>N ligands. This Cu<sub>4</sub>I<sub>4</sub> geometry differs significantly from the âcubaneâ
and âstairstepâ geometries reported for other Cu<sub>4</sub>I<sub>4</sub>L<sub>4</sub> clusters. Luminescence spectra
of clusters <b>3</b> and <b>4</b> display a single emission
around 460 nm at room temperature that is assigned to emission from
a triplet halide-to-ligand charge-transfer (<sup>3</sup>XLCT) excited
state, whereas clusters <b>1</b>, <b>2</b>, and <b>5</b> also have a second band around 570 nm that is assigned to
a Cu<sub>4</sub>I<sub>4</sub> cluster-centered (<sup>3</sup>CC) excited
state. The structural and photophysical properties of a dinuclear
Cu<sub>2</sub>I<sub>2</sub>(P<sup>â§</sup>N)<sub>2</sub> complex
obtained during the sublimation of cluster <b>3</b> is also
provided
In Situ Observation of Degradation by Ligand Substitution in Small-Molecule Phosphorescent Organic Light-Emitting Diodes
Solutions of facial-trisÂ(1-phenylpyrazole)ÂIrÂ(III)
(<i>fac</i>-IrÂ(ppz)<sub>3</sub>), when dissolved in either <i>tert</i>-butyl isocyanide or in solid films of 2-naphthylisocyanide,
undergo
replacement of a ppz ligand by the isocyanide molecules after irradiation
with UV light as demonstrated by liquid chromatograph mass spectrometer
analysis. Similarly, solutions of IrÂ(ppz)<sub>3</sub> and bathophenanthroline
(BPhen) in CH<sub>2</sub>Cl<sub>2</sub> or acetone-<i>d</i><sub>6</sub> form a brightly emissive species, [IrÂ(ppz)<sub>2</sub>(Bphen)]<sup>+</sup> when irradiated with UV light as established
by optical, mass, and <sup>1</sup>H nuclear magnetic resonance spectroscopy.
Electroluminescent data from blocked organic light-emitting diode
(OLED) devices demonstrate that both <i>mer</i>- and <i>fac</i>-(IrÂ(ppz)<sub>3</sub>) dissociate a ligand and coordinate
a neighboring BPhen molecule when the device is operated at moderate
to high current levels. These experiments offer direct evidence of
the dissociation of a metalâligand bond and subsequent ligand
substitution as a degradation pathway in active OLED devices during
operation and provide a route to assay in situ the stability of future
dopants
Manipulating Triplet Yield through Control of Symmetry-Breaking Charge Transfer
The
efficiency of an organic solar cell depends on the efficacy
of exciton diffusion and dissociation processes, and this can be enhanced
by reducing the exciton binding energy and increasing the exciton
lifetime. Zinc chlorodipyrrin (ZCl) complexes exhibit reduced exciton
binding energy due to ultrafast generation of intramolecular charge
transfer (ICT) states via symmetry-breaking charge transfer in polar
media. This Letter explores the fate of the ICT states using nanosecond
transient absorption. In cyclohexane, ZCl undergoes intersystem crossing
to produce triplets with âŒ8 ns time constant (âŒ30% yield),
and no ICT states are generated. However, in more polar solvents,
triplets are generated within 1 ns via ICT state recombination with
âŒ3 times higher yield than produced via ISC. This high triplet
yield in toluene (89%) and acetonitrile (76%) via ICT state recombination
is a beneficial pathway to spin-protect the excited-state decay for
additional charge generation from triplet excited states
Aqueous Colloidal Acene Nanoparticles: A New Platform for Studying Singlet Fission
Singlet
fission is a process that occurs in select molecular systems
wherein a singlet excited state divides its energy to form two triplet
excitations on neighboring chromophores. While singlet fission has
been largely studied in molecular crystals, colloidal nanoparticles
offer the ability to investigate fission using liquid suspensions,
allowing questions regarding the importance of molecular arrangement
and charge transfer to be assessed. Herein, we report the synthesis
of aqueous colloidal nanoparticles of 5,12-diphenyltetracene (DPT),
a material recently demonstrated to undergo singlet fission in disordered
films. Upon synthesis, nanoparticles display absorption features that
lie between those of monomeric DPT and disordered DPT films. These
features evolve over a few days in a manner that suggests an increase
in the degree of association between neighboring molecules within
the nanoparticles. Transient absorption and time-resolved emission
experiments indicate that photoexcited DPT nanoparticles undergo fission,
but produce a lower triplet yield than disordered films
Tandem and Triple-Junction Polymer:Nanocrystal Hybrid Solar Cells Consisting of Identical Subcells
Tandem and triple-junction polymer:nanocrystal
hybrid solar cells
with identical subcells based on P3HT:CdSe nanocrystal bulk heterojunctions
(BHJs) are reported for the first time showing 2-fold and 3-fold increases
of open-circuit voltage (<i>V</i><sub>OC</sub>), respectively,
relative to the single-junction cell. A combination of nanocrystalline
ZnO and pH-neutral PEDOT:PSS is used as the interconnecting layer,
and the thicknesses of subcells are optimized with the guidance of
optical simulations. As a result, the average power conversion efficiency
(PCE) exhibits a significant increase from 2.0% (<i>V</i><sub>OC</sub> = 0.57 V) in single-junction devices to 2.7% (champion
3.1%, <i>V</i><sub>OC</sub> = 1.28 V) in tandem devices
and 2.3% (<i>V</i><sub>OC</sub> = 1.98 V) in triple-junction
devices
Phosphorescence versus Thermally Activated Delayed Fluorescence. Controlling SingletâTriplet Splitting in Brightly Emitting and Sublimable Cu(I) Compounds
Photophysical properties of two highly
emissive three-coordinate
CuÂ(I) complexes, (IPr)ÂCuÂ(py<sub>2</sub>-BMe<sub>2</sub>) (<b>1</b>) and (Bzl-3,5Me)ÂCuÂ(py<sub>2</sub>-BMe<sub>2</sub>) (<b>2</b>), with two different N-heterocyclic (NHC) ligands were investigated
in detail (IPr = 1,3-bisÂ(2,6-diisopropylphenyl)Âimidazol-2-ylidene;
Bzl-3,5Me = 1,3-bisÂ(3,5-dimethylphenyl)-1<i>H</i>-benzoÂ[<i>d</i>]Âimidazol-2-ylidene; py<sub>2</sub>-BMe<sub>2</sub> = diÂ(2-pyridyl)Âdimethylborate).
The compounds exhibit remarkably high emission quantum yields of more
than 70% in the powder phase. Despite similar chemical structures
of both complexes, only compound <b>1</b> exhibits thermally
activated delayed blue fluorescence (TADF), whereas compound <b>2</b> shows a pure, yellow phosphorescence. This behavior is related
to the torsion angles between the two ligands. Changing this angle
has a huge impact on the energy splitting between the first excited
singlet state S<sub>1</sub> and triplet state T<sub>1</sub> and therefore
on the TADF properties. In addition, it was found that, in both compounds,
spinâorbit coupling (SOC) is particularly effective compared
to other CuÂ(I) complexes. This is reflected in short emission decay
times of the triplet states of only 34 ÎŒs (<b>1</b>) and
21 ÎŒs (<b>2</b>), respectively, as well as in the zero-field
splittings of the triplet states amounting to 4 cm<sup>â1</sup> (0.5 meV) for <b>1</b> and 5 cm<sup>â1</sup> (0.6 meV)
for <b>2</b>. Accordingly, at ambient temperature, compound <b>1</b> exhibits <i>two</i> radiative decay paths which
are thermally equilibrated: one via the S<sub>1</sub> state as TADF
path (62%) and one via the T<sub>1</sub> state as phosphorescence
path (38%). Thus, if this material is applied in an organic light-emitting
diode, the generated excitons are harvested mainly in the singlet
state, but to a significant portion also in the triplet state. This
novel mechanism based on two separate radiative decay paths reduces
the overall emission decay time distinctly
High-Efficiency BODIPY-Based Organic Photovoltaics
A benzannulated boron dipyrromethene
(BODIPY, bDIP) molecule exhibiting
strong absorption at 640 nm was synthesized. The organic dye was used
in an organic solar cell as the electron donor with C<sub>60</sub> as the acceptor. The BODIPY dye demonstrated the best performance
in lamellar architecture (indium tin oxide (ITO)/bDIP/C<sub>60</sub>/bathocuproine/Al), giving power conversion efficiency up to 4.5%
with short-circuit current (<i>J</i><sub>SC</sub>) of 8.7
mA/cm<sup>2</sup> and an open-circuit voltage (<i>V</i><sub>OC</sub>) of 0.81 V. Neutron reflectivity experiments were performed
on the bilayer film to investigate the thickness dependence of <i>J</i><sub>SC</sub>. A 13 nm mixed layer was found to be present
at the donor/acceptor interface
in the bilayer device, formed when the C<sub>60</sub> was deposited
onto a room temperature bDIP film. Planar-mixed heterojunction devices
were fabricated to understand the extent of spontaneous mixing between
the donor and acceptor materials. The native mixed region in the bilayer
device was shown to most resemble 1:3 bDIP:C<sub>60</sub> layer in
the structure: (ITO/bDIP/bDIP:C<sub>60</sub> blend/C<sub>60</sub>/bathocuproine/Al)
Dependence of Phosphorescent Emitter Orientation on Deposition Technique in Doped Organic Films
Dependence of Phosphorescent Emitter Orientation on
Deposition Technique in Doped Organic Film