20 research outputs found
Tuning the Photophysical Properties of Homoleptic Tris-Cyclometalated Ir(III) Complexes by Facile Modification of the Imidazo-Phenanthridine and Their Application to Phosphorescent Organic Light-Emitting Diodes
To explore the excited-state
electronic structure of the blue-emitting
Ir(dmp)3 dopant material (dmp = 3-(2,6-dimethylphenyl)-7-methylimidazo[1,2-f]phenanthridine), which is notable for durable blue phosphorescent
organic light-emitting diode (PhOLED), a series of homoleptic dmp-based
Ir(III) complexes (DMP–R, tris[3-(2,6-dimethylphenyl)-7-R-imidazo[1,2-f]phenanthridin-12-yl-κC12,κN1]iridium, R = H, CH3, F, and CF3) were prepared
by introducing an electron-donating group (EDG; −CH3) or an electron-withdrawing group (EWG; −F and −CF3) at the 7-position of the imidazo-phenanthridine ligand.
The photophysical analysis demonstrated that the alteration from EDG
to EWGs led to redshifted structureless emission profiles, which were
correlated with variations in the 3MLCT/3ILCT
ratio in the T1 excited state. From electrochemical studies
and density functional theory calculations, it turned out that the
excited-state nature of the dmp-based Ir(III) complexes was significantly
affected by the inductive effect of the 7-substituent of the cyclometalating
dmp ligand. As a result of the lowest unoccupied molecular orbital
energy stabilization by the EWGs that suppressed the non-radiative
pathway from the emissive triplet excited state to the 3d–d state, the F- and CF3-modified Ir(dmp)3 complexes (DMP–F and DMP–CF3) showed
quantum yields of 27–30% in the solution state, which were
at least 4- or 5-fold higher than those shown by DMP–H and DMP–CH3. A PhOLED
device based on DMP–CF3 [CIE chromaticity (0.17, 0.39)], which demonstrated a distinct 3MLCT characteristic, exhibited better electroluminescent efficiencies
with an external quantum efficiency of 13.5% than that based on DMP–CH3
Tuning the Photophysical Properties of Homoleptic Tris-Cyclometalated Ir(III) Complexes by Facile Modification of the Imidazo-Phenanthridine and Their Application to Phosphorescent Organic Light-Emitting Diodes
To explore the excited-state
electronic structure of the blue-emitting
Ir(dmp)3 dopant material (dmp = 3-(2,6-dimethylphenyl)-7-methylimidazo[1,2-f]phenanthridine), which is notable for durable blue phosphorescent
organic light-emitting diode (PhOLED), a series of homoleptic dmp-based
Ir(III) complexes (DMP–R, tris[3-(2,6-dimethylphenyl)-7-R-imidazo[1,2-f]phenanthridin-12-yl-κC12,κN1]iridium, R = H, CH3, F, and CF3) were prepared
by introducing an electron-donating group (EDG; −CH3) or an electron-withdrawing group (EWG; −F and −CF3) at the 7-position of the imidazo-phenanthridine ligand.
The photophysical analysis demonstrated that the alteration from EDG
to EWGs led to redshifted structureless emission profiles, which were
correlated with variations in the 3MLCT/3ILCT
ratio in the T1 excited state. From electrochemical studies
and density functional theory calculations, it turned out that the
excited-state nature of the dmp-based Ir(III) complexes was significantly
affected by the inductive effect of the 7-substituent of the cyclometalating
dmp ligand. As a result of the lowest unoccupied molecular orbital
energy stabilization by the EWGs that suppressed the non-radiative
pathway from the emissive triplet excited state to the 3d–d state, the F- and CF3-modified Ir(dmp)3 complexes (DMP–F and DMP–CF3) showed
quantum yields of 27–30% in the solution state, which were
at least 4- or 5-fold higher than those shown by DMP–H and DMP–CH3. A PhOLED
device based on DMP–CF3 [CIE chromaticity (0.17, 0.39)], which demonstrated a distinct 3MLCT characteristic, exhibited better electroluminescent efficiencies
with an external quantum efficiency of 13.5% than that based on DMP–CH3
Tuning the Photophysical Properties of Homoleptic Tris-Cyclometalated Ir(III) Complexes by Facile Modification of the Imidazo-Phenanthridine and Their Application to Phosphorescent Organic Light-Emitting Diodes
To explore the excited-state
electronic structure of the blue-emitting
Ir(dmp)3 dopant material (dmp = 3-(2,6-dimethylphenyl)-7-methylimidazo[1,2-f]phenanthridine), which is notable for durable blue phosphorescent
organic light-emitting diode (PhOLED), a series of homoleptic dmp-based
Ir(III) complexes (DMP–R, tris[3-(2,6-dimethylphenyl)-7-R-imidazo[1,2-f]phenanthridin-12-yl-κC12,κN1]iridium, R = H, CH3, F, and CF3) were prepared
by introducing an electron-donating group (EDG; −CH3) or an electron-withdrawing group (EWG; −F and −CF3) at the 7-position of the imidazo-phenanthridine ligand.
The photophysical analysis demonstrated that the alteration from EDG
to EWGs led to redshifted structureless emission profiles, which were
correlated with variations in the 3MLCT/3ILCT
ratio in the T1 excited state. From electrochemical studies
and density functional theory calculations, it turned out that the
excited-state nature of the dmp-based Ir(III) complexes was significantly
affected by the inductive effect of the 7-substituent of the cyclometalating
dmp ligand. As a result of the lowest unoccupied molecular orbital
energy stabilization by the EWGs that suppressed the non-radiative
pathway from the emissive triplet excited state to the 3d–d state, the F- and CF3-modified Ir(dmp)3 complexes (DMP–F and DMP–CF3) showed
quantum yields of 27–30% in the solution state, which were
at least 4- or 5-fold higher than those shown by DMP–H and DMP–CH3. A PhOLED
device based on DMP–CF3 [CIE chromaticity (0.17, 0.39)], which demonstrated a distinct 3MLCT characteristic, exhibited better electroluminescent efficiencies
with an external quantum efficiency of 13.5% than that based on DMP–CH3
Tuning the Photophysical Properties of Homoleptic Tris-Cyclometalated Ir(III) Complexes by Facile Modification of the Imidazo-Phenanthridine and Their Application to Phosphorescent Organic Light-Emitting Diodes
To explore the excited-state
electronic structure of the blue-emitting
Ir(dmp)3 dopant material (dmp = 3-(2,6-dimethylphenyl)-7-methylimidazo[1,2-f]phenanthridine), which is notable for durable blue phosphorescent
organic light-emitting diode (PhOLED), a series of homoleptic dmp-based
Ir(III) complexes (DMP–R, tris[3-(2,6-dimethylphenyl)-7-R-imidazo[1,2-f]phenanthridin-12-yl-κC12,κN1]iridium, R = H, CH3, F, and CF3) were prepared
by introducing an electron-donating group (EDG; −CH3) or an electron-withdrawing group (EWG; −F and −CF3) at the 7-position of the imidazo-phenanthridine ligand.
The photophysical analysis demonstrated that the alteration from EDG
to EWGs led to redshifted structureless emission profiles, which were
correlated with variations in the 3MLCT/3ILCT
ratio in the T1 excited state. From electrochemical studies
and density functional theory calculations, it turned out that the
excited-state nature of the dmp-based Ir(III) complexes was significantly
affected by the inductive effect of the 7-substituent of the cyclometalating
dmp ligand. As a result of the lowest unoccupied molecular orbital
energy stabilization by the EWGs that suppressed the non-radiative
pathway from the emissive triplet excited state to the 3d–d state, the F- and CF3-modified Ir(dmp)3 complexes (DMP–F and DMP–CF3) showed
quantum yields of 27–30% in the solution state, which were
at least 4- or 5-fold higher than those shown by DMP–H and DMP–CH3. A PhOLED
device based on DMP–CF3 [CIE chromaticity (0.17, 0.39)], which demonstrated a distinct 3MLCT characteristic, exhibited better electroluminescent efficiencies
with an external quantum efficiency of 13.5% than that based on DMP–CH3
Tuning the Photophysical Properties of Homoleptic Tris-Cyclometalated Ir(III) Complexes by Facile Modification of the Imidazo-Phenanthridine and Their Application to Phosphorescent Organic Light-Emitting Diodes
To explore the excited-state
electronic structure of the blue-emitting
Ir(dmp)3 dopant material (dmp = 3-(2,6-dimethylphenyl)-7-methylimidazo[1,2-f]phenanthridine), which is notable for durable blue phosphorescent
organic light-emitting diode (PhOLED), a series of homoleptic dmp-based
Ir(III) complexes (DMP–R, tris[3-(2,6-dimethylphenyl)-7-R-imidazo[1,2-f]phenanthridin-12-yl-κC12,κN1]iridium, R = H, CH3, F, and CF3) were prepared
by introducing an electron-donating group (EDG; −CH3) or an electron-withdrawing group (EWG; −F and −CF3) at the 7-position of the imidazo-phenanthridine ligand.
The photophysical analysis demonstrated that the alteration from EDG
to EWGs led to redshifted structureless emission profiles, which were
correlated with variations in the 3MLCT/3ILCT
ratio in the T1 excited state. From electrochemical studies
and density functional theory calculations, it turned out that the
excited-state nature of the dmp-based Ir(III) complexes was significantly
affected by the inductive effect of the 7-substituent of the cyclometalating
dmp ligand. As a result of the lowest unoccupied molecular orbital
energy stabilization by the EWGs that suppressed the non-radiative
pathway from the emissive triplet excited state to the 3d–d state, the F- and CF3-modified Ir(dmp)3 complexes (DMP–F and DMP–CF3) showed
quantum yields of 27–30% in the solution state, which were
at least 4- or 5-fold higher than those shown by DMP–H and DMP–CH3. A PhOLED
device based on DMP–CF3 [CIE chromaticity (0.17, 0.39)], which demonstrated a distinct 3MLCT characteristic, exhibited better electroluminescent efficiencies
with an external quantum efficiency of 13.5% than that based on DMP–CH3
Synthesis and Characterization of Blue Phosphorescent NHC-Ir(III) Complexes with Annulated Heterocyclic 1,2,4-Triazolophenanthridine Derivatives for Highly Efficient PhOLEDs
Efficient tris-bidentate Ir(III)
phosphorescent dopants were prepared
using a series of 1,2,4-triazolo[4,3-f]phenanthridine
(tzp) moieties modified with aryl substituents (phenyl, tolyl, and
xylenyl) as the main phenylimidazole-based N-heterocyclic carbene
(NHC) chelates (C∧C:). According to the degree of
the bulkiness of the aryl substituent and the ligation mode, the five
prepared Ir(tzpC∧C:) complexes include
four homoleptic NHC-Ir(III) complexes, fac-Ir(tzpPh)3, fac-/mer-Ir(tzpTol)3, and mer-Ir(tzpXyl)3, and
one heteroleptic NHC-Ir(III) complex, cis-Ir(tzpPh)2(tzpPh)′, in which the
phenyl moiety of one tzpPh ligand is abnormally ligated to the Ir
metal center, unlike other tzp ligands. The Ir(III) complexes ligated
by carbene ligands (tzpC∧C:) exhibited
highly efficient emissions in the solid state (Φem = 23.2–54.0%). Electrochemical and theoretical studies revealed
that the excited-state properties of these NHC-Ir(III) complexes are
variable on the extent of planarity and π-conjugation of the tzpC∧C: chelating ligand. Due to its enhanced
rigidity and low excited-state energy, a result of abnormal tzpPh
ligand ligation, the heteroleptic cis-Ir(tzpPh)2(tzpPh)′ exhibited the
most efficient emission properties in solution (Φem = 21.4%) and solid (Φem = 54.0%) media. Of the
devices fabricated with Ir(tzpC∧C:)3 complexes as emitters, that doped with cis-Ir(tzpPh)2(tzpPh)′ exhibited superior electroluminescence efficiencies (external quantum
efficiency (EQE) of 16.3%, current efficiency of 27.6 cd A–1, and power efficiency of 22.1 lm W–1) and CIE
coordinates of [0.17,0.26], which are superior to those of other Ir(tzpC∧C:)3 complexes and Ir(dmp)3 (dmp = 3-(2,6-dimethylphenyl)-7-methylimidazo[1,2-f]phenanthridine). This study provides insight into the
molecular-level engineering of Ir(III) dopant materials for improving
the emission efficiencies of phosphorescent OLEDs
Excited-State Modification of Phenylimidazole-Based Cyclometalated Ir(III) Complexes through Secondary Bulky Aryl Substitution and Inductive Modification Enhances the Blue Emission Efficiency in Phosphorescent OLEDs
To elucidate the key parameters governing the emission
properties
of phenylimidazole (pim)-based Ir(III) emitters, including their electronic
structure and the bulky aryl substitution effect, a series of pim-based
iridium(III) complexes (Ir(Rpim-X)3, Rpim-X = 1-R-2-(X-phenyl)-1H-imidazole) bearing secondary pendants of increasing bulkiness [R
= methyl (Me), phenyl (Ph), terphenyl (TPh), or 4-isopropyl terphenyl
(ITPh)] and three different primary pim ligands (X = F, F2, and CN) were designed and synthesized. Based on photophysical and
electrochemical analyses, it was found that the excited state properties
are highly dependent on the bulkiness of the secondary substituent
and the inductive nature of the primary pim ligand. The incorporation
of bulky TPh/ITPh substituents in the second coordination sphere significantly
enhanced the emission efficiencies in the solid state (ΦPL = 72.1–84.9%) compared to those of the methyl- or
phenyl-substituted Ir(III) complexes (ΦPL = 30.4%
for Ir(Mepim)3 and 63.7% for Ir(Phpim)3). Further modification of
the secondary aryl substituent (Ir(TPhpim)3 → Ir(ITPhpim)3)
through the incorporation of an isopropyl group and F substitution
on the primary pim ligand (Ir(TPh/ITPhpim)3 → Ir(TPh/ITPhpim-F/F2)3) resulted in a slight decrease in the LUMO and a significant
decrease in the HOMO energy levels, respectively; these energy level
adjustments consequently amplified emission blue shifts, thereby enabling
efficient blue electroluminescence in phosphorescent organic light-emitting
diodes. Theoretical calculations revealed that the excited-state properties
of pim-based Ir(III) complexes can be modulated by the nature of the
peripheral substituent and the presence of an EWG substituent. Among
the fabricated blue-emitting TPh/ITPh-substituted Ir(III) complexes, Ir(ITPhpim-F)3, Ir(TPhpim-F2)3, and Ir(ITPhpim-F2)3 were tested as blue-emitting
dopants for blue phosphorescent OLEDs owing to their high solid radiative
quantum yields (ΦPL = 75.9–84.9%). The Ir(ITPhpim-F)3-doped multilayer device
displayed the best performance with a maximum external quantum efficiency
of 21.0%, a maximum current efficiency of 43.6 cd/A, and CIE coordinates
of 0.18 and 0.31
Synthesis and Characterization of Blue Phosphorescent NHC-Ir(III) Complexes with Annulated Heterocyclic 1,2,4-Triazolophenanthridine Derivatives for Highly Efficient PhOLEDs
Efficient tris-bidentate Ir(III)
phosphorescent dopants were prepared
using a series of 1,2,4-triazolo[4,3-f]phenanthridine
(tzp) moieties modified with aryl substituents (phenyl, tolyl, and
xylenyl) as the main phenylimidazole-based N-heterocyclic carbene
(NHC) chelates (C∧C:). According to the degree of
the bulkiness of the aryl substituent and the ligation mode, the five
prepared Ir(tzpC∧C:) complexes include
four homoleptic NHC-Ir(III) complexes, fac-Ir(tzpPh)3, fac-/mer-Ir(tzpTol)3, and mer-Ir(tzpXyl)3, and
one heteroleptic NHC-Ir(III) complex, cis-Ir(tzpPh)2(tzpPh)′, in which the
phenyl moiety of one tzpPh ligand is abnormally ligated to the Ir
metal center, unlike other tzp ligands. The Ir(III) complexes ligated
by carbene ligands (tzpC∧C:) exhibited
highly efficient emissions in the solid state (Φem = 23.2–54.0%). Electrochemical and theoretical studies revealed
that the excited-state properties of these NHC-Ir(III) complexes are
variable on the extent of planarity and π-conjugation of the tzpC∧C: chelating ligand. Due to its enhanced
rigidity and low excited-state energy, a result of abnormal tzpPh
ligand ligation, the heteroleptic cis-Ir(tzpPh)2(tzpPh)′ exhibited the
most efficient emission properties in solution (Φem = 21.4%) and solid (Φem = 54.0%) media. Of the
devices fabricated with Ir(tzpC∧C:)3 complexes as emitters, that doped with cis-Ir(tzpPh)2(tzpPh)′ exhibited superior electroluminescence efficiencies (external quantum
efficiency (EQE) of 16.3%, current efficiency of 27.6 cd A–1, and power efficiency of 22.1 lm W–1) and CIE
coordinates of [0.17,0.26], which are superior to those of other Ir(tzpC∧C:)3 complexes and Ir(dmp)3 (dmp = 3-(2,6-dimethylphenyl)-7-methylimidazo[1,2-f]phenanthridine). This study provides insight into the
molecular-level engineering of Ir(III) dopant materials for improving
the emission efficiencies of phosphorescent OLEDs
Photoinduced Electron Transfer in a BODIPY-<i>ortho</i>-Carborane Dyad Investigated by Time-Resolved Transient Absorption Spectroscopy
We
report the results of photoinduced electron transfer (PET) in
a novel dyad, in which a boron dipyrromethene (BODIPY) dye is covalently
linked to <i>o</i>-carborane (<i>o</i>-Cb). In
this dyad, BODIPY and <i>o</i>-Cb act as electron donor
and acceptor, respectively. PET dynamics were investigated using a
femtosecond time-resolved transient absorption spectroscopic method.
The free energy dependence of PET in the S<sub>1</sub> and S<sub>2</sub> states was examined on the basis of Marcus theory. PET in the S<sub>1</sub> state occurs in the Marcus normal region. Rates are strongly
influenced by the driving force (−Δ<i>G</i>), which is controlled by solvent polarity; thus, PET in the S<sub>1</sub> state is faster in polar solvents than in nonpolar ones.
However, PET does not occur from the higher energy S<sub>2</sub> state
despite large endothermic Δ<i>G</i> values, because
deactivation via internal conversion is much faster than PET
Elucidation of Excited-State Properties of Bimetallic Ir(III)–Pt(II) Complexes with Conjugated Bridging Ligands
We
investigated excited-state properties of 4′,7′-phenanthrolino-5′,6′:2,3-pyrazine
(ppz)-bridged bimetallic complexes, (L)2Ir-ppz-PtCl2 (Ir-ppz-Pt) (L = 2-(4′,6′-difluorophenyl)pyridinato-N,C2 (dfppy)), and [(L)2Ir]2(ppz) (Ir-ppz-Ir).
These properties were compared to those of reported dpp bridging complexes, 2,3-bis(2-pyridyl)pyrazine (dpp)-bridged bimetallic complexes, Ir-dpp-Pt, and Ir-dpp-Ir. Excited-state properties of hetero-bimetallic Ir–Pt
systems were very different from those of related Ru–Pt systems
with a dpp bridging ligand; Ru-dpp-Pt displayed
the spin forbidden metal-to-ligand charge-transfer emission, whereas
Ir-dpp-Pt was relatively silent in emission. Steady-state
photochemical studies and photodynamic studies were undertaken for
each Ir or Pt center within peripheries of bridging ligands to confirm
either energy or ET and at the same time its direction. Thermodynamic
driving force of the electron-transfer (ET) process from Ir to Pt
in the hetero-bimetallic Ir–Pt systems was predicted by the
Rehm–Weller equation to be unfavorable for both Ir-ppz-Pt and Ir-dpp-Pt. However, when photoinduced ET in
ground state was considered, the complexes could undergo an ET process
from Pt to Ir center. Such a prediction is well manifested from selective
excitation on the bridging ligand
