Fine-tuning of interfacial adhesion between fillers and polymer matrices is crucial to the separation performance of mixed matrix membranes (MMMs) and their mechanical properties.Direct incorporation of metal organic framework (MOF) particles in polymers often leads to insufficient adhesion and non-selective interfacial voids. Herein, we present a novel strategy to develop toughened MOF-polymer interface by confining a room temperature ionic liquid (IL)[bmim][Tf 2 N] into ZIF-8 cages. The diffusion of the IL out of the IL-incorporated ZIF-8

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The diatomic catalysts (DACs) provide a new strategy for efficient catalysis of CO2 reduction reaction (CO2RR) owing to their maximum atomic utility and more flexible active sites. However, it is...

Here we report a highly scalable yet flexible triple-layer structured porous C/SiO2 membrane via a facile phase inversion method for advancing Li–sulfur battery technology. As a multifunctional current-collector-free cathode, the conductive dense layer of the C/SiO2 membrane offers hierarchical macropores as an ideal sulfur host to alleviate the volume expansion of sulfur species and facilitate ion/electrolyte transport for fast kinetics, as well as spongelike pores to enable high sulfur loading. The triple-layer structured membrane cathode enables the filling of most sulfur species in the macropores and additional loading of a thin sulfur slurry on the membrane surface, which facilitates ion/electrolyte transport with faster kinetics than the conventional S/C slurry-based cathode. Furthermore, density functional theory simulations and visual adsorption measurements confirm the critical role of the doped SiO2 nanoparticles (∼10 nm) in the asymmetric C membrane in suppressing the shuttle effect of polysulfides via chemisorption and electrocatalysis. The rationally designed C/SiO2 membrane cathodes demonstrate long-term cycling stability of 300 cycles at a high sulfur loading of 2.8 mg cm–2 with a sulfur content of ∼75%. This scalable yet flexible self-supporting cathode design presents a useful strategy for realizing practical applications of high-performance Li–S batteries.

Organic light-emitting diodes (OLEDs) have great potential for applications such as flat panel displays and solid-state lighting. [1][2][3][4][5][6] Many green-and red-light-emitting organic materials have been developed for full-color displays but highly efficient and stable blue-light-emitting organic materials are still rare. [7][8][9][10] Due to the large band-gap of blue-light emitters, it is difficult to inject holes from the anode as well as electrons from the cathode in blue-light OLEDs. Promising candidates for blue-light-emitting materials include fluorene-based polymers and oligomers, due to their high photoluminescent quantum yield (PLQY), good thermal stability, and excellent solubility. [11][12][13] In this communication, we report a series of new blue-light-emitting materials consisting of oligofluorenyl blocks and electron-donating/electron-withdrawing groups, which facilitate the injection and transport of both holes and electrons. The device performance of undoped and doped devices indicates that they are very promising for OLEDs, with essential elements of high efficiency, good stability, and color purity for pure-blue emission.The target blue-light-emitting compounds were synthesized through three key steps (Scheme 1). First, 4-iodoaniline was coupled with carbazole through an Ullmann coupling reaction. In our first attempt, where N,N-dimethylacetamide (DMAc) was used as solvent, the reaction solution was heated at 160 8C for 24 h, and 76% yield of compound A was achieved. In our second attempt with diphenyl ether as solvent, the temperature was raised to 190 8C and the reaction yielded 92% of desired product. Compound A was then coupled with dibromo-oligofluorene (B1-B3), catalyzed by Pd(OAc) 2 , to afford compounds C1 to C3, which were eventually end-capped with cyanophenyl groups through a Suzuki coupling reaction. The three coupling reactions produced an overall yield of 55%, 37%, and 33% for D1, D2, and D3, respectively.The physical properties of the compounds are summarized in Table 1. All three compounds show high photoluminescent quantum yields, ranging from 59% to 64% in chloroform solution. With the number of fluorene units increasing from 1 to 3, the optical properties change remarkably. The optical bandgaps determined from the l 0-0 absorption-band edge are 2.78, 2.81, and 2.89 eV for D1, D2 and D3, respectively. The absorption maximum in the UV-vis spectrum of D3 in chloroform solution is blue-shifted by 9 nm, and the peak of photoluminescence (PL) spectrum of the thin film is largely blue-shifted by 33 nm compared with D1, as shown in Figure 1a. The OLED device performances also depend on the number of fluorene units, which will be described below.The preparation of the electroluminescent devices is briefly described as follows (see Experimental section): poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) and the light-emitting layer were spin-coated from solutions onto indium tin oxide (ITO) surfaces sequentially. 1,3,5-tris(phenyl-2-benzimidazolyl)benzene (TPBI...

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Based on the results of first‐principles calculations of the electronic properties of blue light‐emitting materials, the molecular structures of oligofluorenes are optimized by incorporating electron‐withdrawing groups into the molecules to balance hole and electron injection and transport for organic light‐emitting diodes (OLEDs). The result is a remarkable improvement in the maximum external quantum efficiency (EQE) of the undoped device from 2.0% to 4.99%. Further optimization of the device configurations and processing procedures, e.g., by changing the thickness of the emitting layer and through thermal annealing treatments, leads to a very high maximum EQE of 7.40% for the undoped sky‐blue device. Finally, by doping the emitter in a suitable host material, 4,4’‐bis(carbazol‐9‐yl)biphenyl (CBP), at the optimal concentration of 6%, pure blue emission with extremely high maximum EQE of 9.40% and Commission Internationale de l’Eclairage (CIE) coordinates of (0.147, 0.139) is achieved.

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