6 research outputs found
In Situ Synthesis of MnS Hollow Microspheres on Reduced Graphene Oxide Sheets as High-Capacity and Long-Life Anodes for Li- and Na-Ion Batteries
Uniform
MnS hollow microspheres in situ crystallized on reduced
graphene oxide (RGO) nanosheets via a facile hydrothermal method.
The MnS/RGO composite material was used as the anode for Na-ion batteries
for the first time and exhibited excellent cycling performance, superior
specific capacity, and great cycle stability and rate capability for
both Li- and Na-ion batteries. Compared with nonencapsulated pure
MnS hollow microspheres, these MnS/RGO nanocomposites demonstrated
excellent charge–discharge stability and long cycle life. Li-ion
storage testing revealed that these MnS/RGO nanocomposites deliver
high discharge–charge capacities of 640 mAh g<sup>–1</sup> at 1.0 A g<sup>–1</sup> after 400 cycles and 830 mAh g<sup>–1</sup> at 0.5 A g<sup>–1</sup> after 100 cycles.
The MnS/RGO nanocomposites even retained a specific capacity of 308
mAh g<sup>–1</sup> at a current density of 0.1 A g<sup>–1</sup> after 125 cycles as the anode for Na-ion batteries. The outstanding
electrochemical performance of the MnS/RGO composite attributed to
the RGO nanosheets greatly improved the electronic conductivity and
efficiently mitigated the stupendous volume expansion during the progress
of charge and discharge
Long-Lived Room Temperature Deep-Red/Near-IR Emissive Intraligand Triplet Excited State (<sup>3</sup>IL) of Naphthalimide in Cyclometalated Platinum(II) Complexes and Its Application in Upconversion
[C<sup>∧</sup>NPtÂ(acac)] (C<sup>∧</sup>N = cyclometalating
ligand; acac = acetylacetonato) complexes in which the naphthalimide
(NI) moiety is directly cyclometalated (NI as the C donor of the C–Pt
bond) were synthesized. With 4-pyrazolylnaphthalimide, isomers with
five-membered (<b>Pt-2</b>) and six-membered (<b>Pt-3</b>) chelate rings were obtained. With 4-pyridinylnaphthalimide, only
the complex with a five-membered chelate ring (<b>Pt-4</b>)
was isolated. A model complex with 1-phenylpyrazole as the C<sup>∧</sup>N ligand was prepared (<b>Pt-1</b>). Strong absorption of visible
light (ε = 21 900 M<sup>–1</sup> cm<sup>–1</sup> at 443 nm for <b>Pt-3</b>) and room temperature (RT) phosphorescence
at 630 nm (<b>Pt-2</b> and <b>Pt-3</b>) or 674 nm (<b>Pt-4</b>) were observed. Long-lived phosphorescences were observed
for <b>Pt-2</b> (τ<sub>P</sub> = 12.8 μs) and <b>Pt-3</b> (τ<sub>P</sub> = 61.9 μs). <b>Pt-1</b> is nonphosphorescent at RT in solution because of the acac-localized
T<sub>1</sub> excited state [based on density functional theory (DFT)
calculations and spin density analysis], but a structured emission
band centered at 415 nm was observed at 77 K. Time-resolved transient
absorption spectra and spin density analysis indicated a NI-localized
intraligand triplet excited state (<sup>3</sup>IL) for complexes <b>Pt-2</b>, <b>Pt-3</b>, and <b>Pt-4</b>. DFT calculations
on the transient absorption spectra (T<sub>1</sub> → T<sub><i>n</i></sub> transitions, <i>n</i> > 1)
also
support the <sup>3</sup>IL assignment of the T<sub>1</sub> excited
states of <b>Pt-2</b>, <b>Pt-3</b>, and <b>Pt-4</b>. The complexes were used as triplet sensitizers for triplet–triplet-annihilation
(TTA) based upconversion, and the results show that <b>Pt-3</b> is an efficient sensitizer with an upconversion quantum yield of
up to 14.1%, despite its low phosphorescence quantum yield of 5.2%.
Thus, we propose that the sensitizer molecules at the triplet excited
state that are otherwise nonphosphorescent were involved in the TTA
upconversion process, indicating that weakly phosphorescent or nonphosphorescent
transition-metal complexes can be used as triplet sensitizers for
TTA upconversion
Facile Soaking Strategy Toward Simultaneously Enhanced Conductivity and Toughness of Self-Healing Composite Hydrogels Through Constructing Multiple Noncovalent Interactions
Tough and stretchable
conductive hydrogels are desirable for the
emerging field of wearable and implanted electronics. Unfortunately,
most existing conductive hydrogels have low mechanical strength. Current
strategies to enhance mechanical properties include employing tough
host gel matrices or introducing specific interaction between conductive
polymer and host gel matrices. However, these strategies often involve
additional complicated processes. Here, a simple yet effective soaking
treatment is employed to concurrently enhance mechanical and conductive
properties, both of which can be facilely tailored by controlling
the soaking duration. The significant improvements are correlated
with co-occurring mechanism of deswelling and multiple noncovalent
interactions. The resulting optimal sample exhibits attractive combination
of high water content (75 wt %), high tensile stress (∼2.5
MPa), large elongation (>600%), reasonable conductivity (∼25
mS/cm), and fast self-healing property with the aid of hot water.
The potential application of gel as a strain sensor is demonstrated.
The applicability of this method is not limited to conductive hydrogels
alone but can also be extended to strengthen other functional hydrogels
with weak mechanical properties
Facile Soaking Strategy Toward Simultaneously Enhanced Conductivity and Toughness of Self-Healing Composite Hydrogels Through Constructing Multiple Noncovalent Interactions
Tough and stretchable
conductive hydrogels are desirable for the
emerging field of wearable and implanted electronics. Unfortunately,
most existing conductive hydrogels have low mechanical strength. Current
strategies to enhance mechanical properties include employing tough
host gel matrices or introducing specific interaction between conductive
polymer and host gel matrices. However, these strategies often involve
additional complicated processes. Here, a simple yet effective soaking
treatment is employed to concurrently enhance mechanical and conductive
properties, both of which can be facilely tailored by controlling
the soaking duration. The significant improvements are correlated
with co-occurring mechanism of deswelling and multiple noncovalent
interactions. The resulting optimal sample exhibits attractive combination
of high water content (75 wt %), high tensile stress (∼2.5
MPa), large elongation (>600%), reasonable conductivity (∼25
mS/cm), and fast self-healing property with the aid of hot water.
The potential application of gel as a strain sensor is demonstrated.
The applicability of this method is not limited to conductive hydrogels
alone but can also be extended to strengthen other functional hydrogels
with weak mechanical properties
Molecular Structure–Intersystem Crossing Relationship of Heavy-Atom-Free BODIPY Triplet Photosensitizers
A thiophene-fused
BODIPY chromophore displays a large triplet-state
quantum yield (Φ<sub>T</sub> = 63.7%). In contrast, when the
two thienyl moieties are not fused into the BODIPY core, intersystem
crossing (ISC) becomes inefficient and Φ<sub>T</sub> remains
low (Φ<sub>T</sub> = 6.1%). First-principles calculations including
spin–orbit coupling (SOC) were performed to quantify the ISC.
We found larger SOC and smaller singlet–triplet energy gaps
for the thiophene-fused BODIPY derivative. Our results are useful
for studies of the photochemistry of organic chromophores
Different Quenching Effect of Intramolecular Rotation on the Singlet and Triplet Excited States of Bodipy
It
is well-known that the fluorescence of a chromophore can be efficiently
quenched by the free rotor effect, sometimes called intramolecular
rotation (IMR), i.e. by a large-amplitude torsional motion. Using
this effect, aggregation induced enhanced emission (AIE) and fluorescent
molecular probes for viscosity measurements have been devised. However,
the rotor effect on triplet excited states was rarely studied. Herein,
with molecular rotors of Bodipy and diiodoBodipy, and by using steady
state and time-resolved transient absorption/emission spectroscopies,
we confirmed that the triplet excited state of the Bodipy chromophore
is not quenched by IMR. This is in stark contrast to the fluorescence
(singlet excited state), which is significantly quenched by IMR. This
result is rather interesting since a long-lived excited state (triplet,
276 μs) is not quenched by the IMR, but the short-lived excited
state (singlet, 3.8 ns) is quenched by the same IMR. The unquenched
triplet excited state of the Bodipy was used for triplet–triplet
annihilation upconversion, and the upconversion quantum yield is 6.3%