presence of aliphatic ligands. [ 7 ] These perovskite nanocrystals are highly luminescent and emit over the full visible range, making them ideal candidates for luminescent display applications. [ 6 ] The synthetic steps are generally straightforward, and the easy control of halide content allows the perovskite bandgaps to be tailored, both by chemical compositions as well as by quantum size effects. So far, perovskite nanocrystals are shown to have color-pure emission, close to unity photoluminescence yield and low lasing thresholds. [ 8 ] These nanocrystals were also attempted in light-emitting devices, but effi ciencies remain modest at 0.12%. [ 9 ] Here, we show the preparation of highly effi cient perovskite light-emitting diodes (PeLED) using solution-processed nanocrystals. We apply a new trimethylaluminum (TMA) vapor-based crosslinking method to render the nanocrystal fi lms insoluble, thereby allowing the deposition of subsequent charge-injection layers without the need for orthogonal solvents. The resulting near-complete nanocrystal fi lm coverage, coupled with the natural confi nement of injected charges within the perovskite crystals, facilitate electron-hole capture and give rise to a remarkable electroluminescence yield of 5.7%. Here, our electron-injection layer comprises a fi lm of zinc oxide (ZnO) nanocrystals, directly deposited on an indium tin oxide (ITO)-coated glass substrate. [ 4 ] The cesium lead halide nanocrystals were solution-coated onto the ZnO fi lm as the emissive layer. Due to the presence of aliphatic ligands on the nanocrystals, the perovskite fi lm remains soluble to organic solvents, which limits the deposition of subsequent chargeinjection layers using solution methods. We employed a new TMA vapor-phase crosslinking technique to fi x the nanocrystal fi lm in place, thereby enabling us to solution-cast a layer of TFB polymer (poly[(9,9-dioctylfl uorenyl-2,7-diyl)-co -(4,4′-( N -(4-sec-butylphenyl)diphenylamine)]) above without washing the nanocrystals off. TFB serves primarily as a hole-injection and electron-blocking layer. A thin, high work-function molybdenum trioxide (MoO 3 ) interlayer and silver electrode were vacuum-thermal evaporated to complete the device.As shown in Figure 1 c,d, our perovskite nanocrystal devices show saturated and color-pure emission. We control the perovskite bandgap, primarily by tailoring the halide composition, and achieve electroluminescence across a wide range of the visi ble spectrum. Our red, orange, green, and blue devices emit at wavelengths of 698, 619, 523, and 480 nm, respectively.

A novel type of flexible fiber/wearable supercapacitor that is composed of two fiber electrodes - a helical spacer wire and an electrolyte - is demonstrated. In the carbon-based fiber supercapacitor (FSC), which has high capacitance performance, commercial pen ink is directly utilized as the electrochemical material. FSCs have potential benefits in the pursuit of low-cost, large-scale, and efficient flexible/wearable energy storage systems.

For modern color-rendering applications, efficient blue, green, and red LEDs are required. While efficient green and red perovskite LEDs have been demonstrated, blue devices lag significantly behind due to the poor quality of chloride-based perovskites. Here, we show that doping manganese into blue perovskite nanocrystals increases their brightness and efficiency. By putting doped nanocrystals into LEDs, we see a 4-fold increase in efficiency, demonstrating that blue LEDs can be as efficient as their red and green cousins.

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Light-emitting diodes utilizing perovskite nanocrystals have generated strong interest in the past several years, with green and red devices showing high efficiencies. Blue devices, however, have lagged significantly behind. Here, it is shown that the device architecture plays a key role in this lag and that NiO , a transport layer in one of the highest efficiency devices to date, causes a significant reduction in perovskite luminescence lifetime. An alternate transport layer structure which maintains robust nanocrystal emission is proposed. Devices with this architecture show external quantum efficiencies of 0.50% at 469 nm, seven times higher than state-of-the-art devices at that wavelength. Finally, it is demonstrated that this architecture enables efficient devices across the entire blue-green portion of the spectrum. The improvements demonstrated here open the door to efficient blue perovskite light-emitting diodes.

Lead halide perovskites have emerged as low-cost, high-performance optical and optoelectronic materials, however, their material stability has been a limiting factor for broad applications. Here, we demonstrate stable core-shell colloidal perovskite nanocrystals using a novel, facile and low-cost copolymer templated synthesis approach. The block copolymer serves as a confined nanoreactor during perovskite crystallization and passivates the perovskite surface by forming a multidentate capping shell, thus significantly improving its photostability in polar solvents. Meanwhile, the polymer nanoshell provides an additional layer for further surface modifications, paving the way to functional nanodevices that can be self-assembled or lithographically defined.

Nitrogen-doped graphene was demonstrated as an efficient and alternative metal-free electrocatalyst for dye-sensitized solar cells. Electrochemical measurements showed that the nitrogen-doping process can remarkably improve the catalytic activity of graphene toward triiodide reduction, lower the charge transfer resistance, and thus enhance the corresponding photovoltaic performance. Furthermore, the nitrogen doping levels ranging from 3.5 at% to 18 at%, as well as the nitrogen states (including pyrrolic, pyridinic and quaternary configurations) in graphene, were controlled to interpret the roles of graphene structure in catalytic activity and device performance. The results suggested that the nitrogen states, rather than the total N content, have a significant effect on the catalytic activity. Both pyridinic and quaternary nitrogen states can provide active sites for promoting triiodide reduction reaction, probably due to the shift in redox potential and the lowered adsorption energy.

Controlling matter-light interactions with cavities is of fundamental importance in modern science and technology [1]. It is exemplified in the strong-coupling regime, where matter-light hybrid modes form, with properties controllable via the photon component on the optical-wavelength scale [2,3]. In contrast, matter excitations on the nanometer scale are harder to access. In twodimensional van der Waals heterostructures, a tunable moiré lattice potential for electronic excitations may form [4], enabling correlated electron gases in lattice potentials [5][6][7][8][9]. Excitons confined in moiré lattices [10,11] have also been reported, but cooperative effects have been elusive and interactions with light have remained perturbative [12][13][14][15]. Here, integrating MoSe 2 -WS 2 heterobilayers in a microcavity, we establish cooperative coupling between moiré -lattice excitons and microcavity photons up to liquid-nitrogen temperature, thereby integrating into one platform versatile control over both matter and light. The density dependence of the moiré polaritons reveals strong nonlinearity due to exciton blockade, suppressed exciton energy shift, and suppressed excitation-induced dephasing, all of which are consistent with the quantum-confined nature of the moiré excitons. Such a moiré polariton system combines strong nonlinearity and microscopic-scale tuning of matter excitations with the power of cavity engineering and long range coherence of light, providing a new platform for collective phenomena from tunable arrays of quantum emitters.