7 research outputs found
Highly Efficient Room-Temperature Phosphorescence from Halogen-Bonding-Assisted Doped Organic Crystals
The
development of metal-free organic room temperature phosphorescence
(RTP) materials has attracted increasing attention because of their
applications in sensors, biolabeling (imaging) agents and anticounterfeiting
technology, but remains extremely challenging owing to the restricted
spin-flip intersystem crossing (ISC) followed by low-yield phosphorescence
that cannot compete with nonradiative relaxation processes. Here,
we report a facile strategy to realize highly efficient RTP by doping
iodo difluoroboron dibenzoylmethane (I-BF<sub>2</sub>dbm-R) derivatives
into a rigid crystalline 4-iodobenzonitrile (Iph-CN) matrix.
We found that halogen bonding between cyano group of Iph-CN
matrix and iodine atom of I-BF<sub>2</sub>dbm-R dopant is formed in
doped crystals, i.e., Iph-CN···I-BF<sub>2</sub>dbm-R, which not only suppresses nonradiative relaxation of triplets
but also promotes the spin–orbit coupling (SOC). As a result,
the doped crystals show intense RTP with an efficiency up to 62.3%.
By varying the substituent group R in I-BF<sub>2</sub>dbm-R from electron
donating −OCH<sub>3</sub> to electron accepting −F,
−CN groups, the ratio between phosphorescence and fluorescence
intensities has been systematically increased from 3.8, 15, to 50
Highly Efficient Room-Temperature Phosphorescence from Halogen-Bonding-Assisted Doped Organic Crystals
The
development of metal-free organic room temperature phosphorescence
(RTP) materials has attracted increasing attention because of their
applications in sensors, biolabeling (imaging) agents and anticounterfeiting
technology, but remains extremely challenging owing to the restricted
spin-flip intersystem crossing (ISC) followed by low-yield phosphorescence
that cannot compete with nonradiative relaxation processes. Here,
we report a facile strategy to realize highly efficient RTP by doping
iodo difluoroboron dibenzoylmethane (I-BF<sub>2</sub>dbm-R) derivatives
into a rigid crystalline 4-iodobenzonitrile (Iph-CN) matrix.
We found that halogen bonding between cyano group of Iph-CN
matrix and iodine atom of I-BF<sub>2</sub>dbm-R dopant is formed in
doped crystals, i.e., Iph-CN···I-BF<sub>2</sub>dbm-R, which not only suppresses nonradiative relaxation of triplets
but also promotes the spin–orbit coupling (SOC). As a result,
the doped crystals show intense RTP with an efficiency up to 62.3%.
By varying the substituent group R in I-BF<sub>2</sub>dbm-R from electron
donating −OCH<sub>3</sub> to electron accepting −F,
−CN groups, the ratio between phosphorescence and fluorescence
intensities has been systematically increased from 3.8, 15, to 50
Organic Phosphorescence Nanowire Lasers
Organic solid-state lasers (OSSLs)
based on singlet fluorescence
have merited intensive study as an important class of light sources.
Although the use of triplet phosphors has led to 100% internal quantum
efficiency in organic light-emitting diodes (OLEDs), stumbling blocks
in triplet lasing include generally forbidden intersystem crossing
(ISC) and a low quantum yield of phosphorescence (Φ<sub>P</sub>). Here, we reported the first triplet-phosphorescence OSSL from
a nanowire microcavity of a sulfide-substituted difluoroboron compound.
As compared with the unsubstituted parent compound, the lone pair
of electrons of sulfur substitution plus the intramolecular charge
transfer interaction introduced by the nitro moiety lead to an highly
efficient T<sub>1</sub> (π,π*) ← S<sub>1</sub> (n,π*)
ISC (Φ<sub>ISC</sub> = 100%) and a moderate Φ<sub>P</sub> (10%). This, plus the optical feedback provided by nanowire Fabry–Perot
microcavity, enables triplet-phosphorescence OSSL emission at 650
nm under pulsed excitation. Our results open the door for a whole
new class of laser materials based on previously untapped triplet
phosphors
Absence of Intramolecular Singlet Fission in Pentacene–Perylenediimide Heterodimers: The Role of Charge Transfer State
A new
class of donor–acceptor heterodimers based on two
singlet fission (SF)-active chromophores, i.e., pentacene (Pc) and
perylenediimide (PDI), was developed to investigate the role of charge
transfer (CT) state on the excitonic dynamics. The CT state is efficiently
generated upon photoexcitation. However, the resulting CT state decays
to different energy states depending on the energy levels of the CT
state. It undergoes extremely rapid deactivation to the ground state
in polar CH<sub>2</sub>Cl<sub>2</sub>, whereas it undergoes transformation
to a Pc triplet in nonpolar toluene. The efficient triplet generation
in toluene is not due to SF but CT-mediated intersystem crossing.
In light of the energy landscape, it is suggested that the deep energy
level of the CT state relative to that of the triplet pair state makes
the CT state actually serve as a trap state that cannot undergoes
an intramolecular singlet fission process. These results provide guidance
for the design of SF materials and highlight the requisite for more
widely applicable design principles
Rational Design of Charge-Transfer Interactions in Halogen-Bonded Co-crystals toward Versatile Solid-State Optoelectronics
Charge-transfer (CT) interactions
between donor (D) and acceptor
(A) groups, as well as CT exciton dynamics, play important roles in
optoelectronic devices, such as organic solar cells, photodetectors,
and light-emitting sources, which are not yet well understood. In
this contribution, the self-assembly behavior, molecular stacking
structure, CT interactions, density functional theory (DFT) calculations,
and corresponding physicochemical properties of two similar halogen-bonded
co-crystals are comprehensively investigated and compared, to construct
an “assembly–structure–CT-property” relationship.
Bpe-IFB wire-like crystals (where Bpe = 1,2-bis(4-pyridyl)ethylene
and IFB = 1,3,5-trifluoro-2,4,6-triiodobenzene), packed in a
segregated stacking form with CT ground and excited states, are measured
to be quasi-one-dimensional (1D) semiconductors and show strong violet-blue
photoluminescence (PL) from the lowest CT<sub>1</sub> excitons (Φ<sub>PL</sub> = 26.1%), which can be confined and propagate oppositely
along the 1D axial direction. In comparison, Bpe-F<sub>4</sub>DIB
block-like crystals (F<sub>4</sub>DIB = 1,4-diiodotetrafluorobenzene),
packed in a mixed stacking form without CT interactions, are determined
to be insulators and exhibit unique white light emission and two-dimensional
optical waveguide property. Surprisingly, it seems that the intrinsic
spectroscopic states of Bpe and F<sub>4</sub>DIB do not change after
co-crystallization, which is also confirmed by theoretical calculations,
thus offering a new design principle for white light emitting materials.
More importantly, we show that the CT interactions in co-crystals
are related to their molecular packing and can be triggered or suppressed
by crystal engineering, which eventually leads to distinct optoelectronic
properties. These results help us to rationally control the CT interactions
in organic D–A systems by tuning the molecular stacking, toward
the development of a fantastic “optoelectronic world”
Self-Assembled Microdisk Lasers of Perylenediimides
Organic solid-state
lasers (OSSLs) have been a topic of intensive
investigations. Perylenediimide (PDI) derivatives are widely used
in organic thin-film transistors and solar cells. However, OSSLs based
on neat PDIs have not been achieved yet, owing to the formation of
H-aggregates and excimer trap-states. Here, we demonstrated the first
PDI-based OSSL from whispering-gallery mode (WGM) hexagonal microdisk
(hMD) microcavity of N,N′-bis(1-ethylpropyl)-2,5,8,11-tetrakis(<i>p</i>-methyl-phenyl)-perylenediimide (<i>mp</i>-PDI)
self-assembled from solution. Single-crystal data reveal that <i>mp</i>-PDI molecules stack into a loosely packed twisted brickstone
arrangement, resulting in J-type aggregates that exhibit a solid-state
photoluminescence (PL) efficiency φ > 15%. Moreover, we found
that exciton-vibration coupling in J-aggregates leads to an exceptional
ultrafast radiative decay, which reduces the exciton diffusion length,
in turn, suppresses bimolecular exciton annihilation (bmEA) process.
These spectral features, plus the optical feedback provided by WGM-hMD
microcavity, enable the observation of multimode lasing as evidenced
by nonlinear output, spectral narrowing, and temporal coherence of
laser emission. With consideration of high carrier-mobility associated
with PDIs, hMDs of <i>mp</i>-PDI are attractive candidates
on the way to achieve electrically driven OSSL
Self-Assembled Microdisk Lasers of Perylenediimides
Organic solid-state
lasers (OSSLs) have been a topic of intensive
investigations. Perylenediimide (PDI) derivatives are widely used
in organic thin-film transistors and solar cells. However, OSSLs based
on neat PDIs have not been achieved yet, owing to the formation of
H-aggregates and excimer trap-states. Here, we demonstrated the first
PDI-based OSSL from whispering-gallery mode (WGM) hexagonal microdisk
(hMD) microcavity of N,N′-bis(1-ethylpropyl)-2,5,8,11-tetrakis(<i>p</i>-methyl-phenyl)-perylenediimide (<i>mp</i>-PDI)
self-assembled from solution. Single-crystal data reveal that <i>mp</i>-PDI molecules stack into a loosely packed twisted brickstone
arrangement, resulting in J-type aggregates that exhibit a solid-state
photoluminescence (PL) efficiency φ > 15%. Moreover, we found
that exciton-vibration coupling in J-aggregates leads to an exceptional
ultrafast radiative decay, which reduces the exciton diffusion length,
in turn, suppresses bimolecular exciton annihilation (bmEA) process.
These spectral features, plus the optical feedback provided by WGM-hMD
microcavity, enable the observation of multimode lasing as evidenced
by nonlinear output, spectral narrowing, and temporal coherence of
laser emission. With consideration of high carrier-mobility associated
with PDIs, hMDs of <i>mp</i>-PDI are attractive candidates
on the way to achieve electrically driven OSSL