5 research outputs found
New Multichannel Frontal Polymerization Strategy for Scaled-up Production of Robust Hydrogels
Herein,
we report a new facile and safe pathway for the scaled-up
production of mechanically strong and multiresponsive interpenetrating
polymer network (IPN) hydrogels via multichannel frontal polymerization
(multichannel FP). We designed a two-part system, of which part-1
contained high reactive monomer and could polymerize spontaneously.
The polymerization of part-1 released tremendous amount of heat, subsequently
initiating FP of part-2 to convert monomers to polymers without any
external energy, which is flexible, cost-effective, and environmental.
Multichannel FP not only allowed realization of parallel polymerization
to obtain a number of hydrogels but also solved center overheating
and explosion problem stemmed from a large reaction vessel. Compared
with the sample prepared in bigger tubular reactor, product synthesized
via multichannel FP showed more excellent thermal stability, morphology
and mechanical properties. Moreover, the as-prepared IPN hydrogels
exhibited chemical-, pH-, and thermal-sensitivity toward various external
changes, which might broaden the applications of hydrogels in sensors
Magnetic-Directed Assembly from Janus Building Blocks to Multiplex Molecular-Analogue Photonic Crystal Structures
The predictable assembly of colloidal
particles into a programmable
superstructure is a challenging and vital task in chemistry and materials
science. In this work, we develop an available magnetic-directed assembly
strategy to construct a series of molecular-analogue photonic crystal
cluster particles involving dot, line, triangle, tetrahedron, and
triangular bipyramid configurations from solid–liquid Janus
building blocks. These versatile multiplex molecular-analogue structural
clusters containing photonic band gap, fluorescent, and magnetic information
can open a new promising access to a variety of robust hierarchical
microstructural particle materials
Fabrication of Reversible Phase Transition Polymer Gels toward Metal Ion Sensing
We
report the synthesis of a new type of triple stimuli-responsive,
i.e., thermo-, pH-, and metal ion-responsive copolymers based on polyÂ(<i>N</i>-vinylimidazole-<i>co</i>-methacrylic acid) (polyÂ(VI-<i>co</i>-MAA)) and their application as metal ion sensors. The
copolymers exhibit reversible sol–gel phase transition behavior
in aqueous media. The sol-to-gel transition temperature (<i>T</i><sub>sol–gel</sub>) can be shifted in the range of 20–80
°C, by varying monomer ratio and feeding glycerol content, by
adjusting the copolymer concentration in aqueous solution, by tuning
the pH of the solution, or by adding various divalent metal ions.
Metal ion sensors were designed upon an inverse opal photonic film
loaded with aqueous solution of polyÂ(VI-<i>co</i>-MAA),
which allows the easy reorganization of various divalent metal ions
by combining the diversity of <i>T</i><sub>sol–gel</sub> of the copolymers on different metal ions and flexible reflection
spectra of the film. In addition, a fluorescent reversible sol–gel
transition system was established by <i>in situ</i> generation
of nanocrystals in the copolymer matrix. These extensions may provide
the multiresponsive copolymers great flexibility for applications
in biomedical, optical, and sensory fields
Design of Phosphor White Light Systems for High-Power Applications
We
developed a strategy that transforms phosphor down-converting
white light sources from low-power systems into efficient high-power
ones. To incorporate multiple phosphors, we generalized and extended
a phosphor layer model, which we term CCAMP (color correction analysis
for multiple phosphors). CCAMP describes both the scattering and saturation
of phosphor materials and allows modeling of different layered structures.
We employed a phosphor mixture comprising YAG:Ce and K<sub>2</sub>TiF<sub>6</sub>:Mn<sup>4+</sup> to illustrate the effectiveness of
the model. YAG:Ce’s high density and small particle size produce
a large amount of scattering, while the long (4.8 ms) photoluminescent
lifetime of K<sub>2</sub>TiF<sub>6</sub>:Mn<sup>4+</sup> results in
saturation at high pump power. By incorporating experimental photophysical
results from the phosphors, we modeled our system and chose the design
suitable for high-power applications. We report the first solid-state
phosphor system that creates warm white light emission at powers up
to 5 kW/cm<sup>2</sup>. Furthermore, at this high power, the system’s
emission achieves the digital cinema initiative (DCI) requirements
with a luminescence efficacy improvement of 20% over the stand-alone
ceramic YAG:Ce phosphor
Quantum Dot Color-Converting Solids Operating Efficiently in the kW/cm<sup>2</sup> Regime
With
rapid progress in the use of colloidal quantum dots (QDs)
as light emitters, the next challenge for this field is to achieve
high brightness. Unfortunately, Auger recombination militates against
high emission efficiency at multiexciton excitation levels. Here,
we suppress the Auger-recombination-induced photoluminescence (PL)
quantum yield (QY) loss in CdSe/CdS core–shell QDs by reducing
the absorption cross section at excitation wavelengths via a thin-shell
design. Studies of PL vs shell thickness reveal that thin-shell QDs
better retain their QY at high excitation intensities, in stark contrast
to thicker-shell QDs. Ultrafast transient absorption spectroscopy
confirms increased Auger recombination in thicker-shell QDs under
equivalent external excitation intensities. We then further grow a
thin ZnS layer on thin-shell QDs to serve as a higher conduction band
barrier; this allows for better passivation and exciton confinement,
while providing transparency at the excitation wavelength. Finally,
we develop an isolating silica matrix that acts as a spacer between
dots, greatly reducing interdot energy transfer that is otherwise
responsible for PL reduction in QD films. This results in the increase
of film PL QY from 20% to 65% at low excitation intensity. The combination
of Auger reduction and elimination of energy transfer leads to QD
film PL QY in excess of 50% and absolute power conversion efficiency
of 28% at excitation powers of 1 kW/cm<sup>2</sup>, the highest ever
reported for QDs under intense illumination