Molecular design of conjugated polymers for efficient electroluminescence (EL) and color tuning has long been one of the most important subjects in the development of polymer light emitting diodes (PLED) and can be carried out in two ways: by chemical and physical methods. The chemical method, involving the incorporation of charge-transport moieties on the main chain, [1][2][3] flexible side chain, [4][5][6] and chain ends, [7] has been extensively studied for poly(phenylene vinylene)s, polyfluorenes, and other polyarylenes in order to promote balanced hole and electron fluxes and to adjust highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) levels, as well as the band gap for color tuning. Taking polyfluorenes as an example, incorporation of triphenylamine in the main chain and oxadiazole in the side chain provides an improvement in the efficiency and purity of blue emission to 2.07 cd A -1 and a Commission Internationale de l'Eclairage (CIE) value of x + y = 0.29, respectively, which is the best blue fluorescence device that has been reported so far.[1] However, chemical methods require elaborate synthesis.Physical methods include blending a conjugated polymer with dopants, [8][9][10] tuning a chain conformation, [11][12][13][14] and manipulating a supramolecular structure.[15] The former involves energy transfer and charge trapping allowing an enhancement of device performance in addition to color tuning and has been studied extensively. Studies on the effects of the tuning of chain conformation on EL are scarce, but studies on the effect of the manipulation of the supramolecular structure on the photoluminescence (PL) of the blue-emitting polymer poly(9,9-di-n-octyl-2,7-fluorene) (PFO) are extensive. Because of its highly coplanar backbone, PFO can be physically transformed by into a variety of supramolecular structures, [11][12][13][14] such as crystalline phases (i.e., a and a′ phase) and noncrystalline phases (such as amorphous, nematic, and b phase, which has an extended conjugation length of about 30repeat units, as evidenced by wide-angle X-ray diffraction).[16]Among these structures, b phase has attracted the most attention because of its specific physical properties, such as a lower extent of triplet exciton formation, [17] a reduced ability to be photobleached on the single-molecule scale, [18] and efficient energy transfer from the amorphous to the b phase. [19] b phase can be physically formed by dissolving PFO in solvents with lower solvent power and higher boiling points [19] or in a solvent/nonsolvent mixture (for example, chloroform/methanol), [20] by exposing a PFO film to solvent vapors (i.e., hexane, cyclohexane, tetrahydrofuran (THF), or toluene), [16] or by applying specific thermal treatment to a PFO film (cooling and reheating to room temperature). [16] In our previous work, [21] we reported that the use of an electron-deficient moiety (such as triazole) as an end-capper for PFO can induce a trace amount of b phase without any further physical treatme...

high photoluminescence quantum yield (PLQY), wide wavelength tunability, and high color purity, [4][5][6] they have been attractive for light-emitting diode (LED) applications. Since the first demonstration of perovskite LEDs in 2014, [7] the device external quantum efficiency (EQE) has risen rapidly from 0.1% [7] to ≈20%, [2,4,8] and the efficiency enhancements are mainly attributed to passivation and compositional engineering, [2,8] improved charge balance by optimization of device structure, [9] and efficient light extraction. [4] More recently, these materials are considered as optical gain medium for lasers. In 2014, the first amplified spontaneous emission (ASE) was observed from CH 3 NH 3 PbI 3 thin films with a threshold of 12 µJ cm −2 and a gain of 250 cm −1 , which is ascribed to the large absorption coefficient, low bulk defect density, and slow Auger recombination rate. [10] These ASE threshold and gain values are comparable to the state of art gain media such as colloidal quantum dots [11] and organic thin films. [12] Since then, optically pumped lasers have been demonstrated based on various microcavity structures such as Fabry-Pérot cavities, [13,14] distributed feedback (DFB) gratings, [3,15] and whispering gallery cavities. [16] The flexibility of fabricating hybrid perovskite lasers using solution-processed methods enables large-scale production and is attractive for the realization of on-chip integration of photonic circuits. [17] Quasi-2D perovskites, which are also known as Ruddlesden-Popper (RP) perovskites, are mixed phases of 2D and 3D nanocrystals. In the mixture, 2D domains exhibit quantumwell-like electronic properties with strong exciton binding energy due to the reduced dimensionality. [18] Typically, the 2D perovskite (A') 2 A n−1 B n X 3n+1 domains consist of multilayers of BX 6 octahedra separated by intercalating ammonium cations A', which is too large to fit into the crystal structure and hinder the growth of 3D ABX 3 crystals (A = methylammonium (MA + ), formamidinium (FA + ), or Cs + , B = Pb 2+ , and X = I − , Br − , Cl − ). As a result, the number of layers determine the bandgap of 2D quantum-well-like domains. [19] Different from 3D perovskites, thin films of qausi-2D perovskites typically contain a mixture of domains with different layers. Within such inhomogenous Quasi-2D Ruddlesden-Popper halide perovskites with a large exciton binding energy, self-assembled quantum wells, and high quantum yield draw attention for optoelectronic device applications. Thin films of these quasi-2D perovskites consist of a mixture of domains having different dimensionality, allowing energy funneling from lower-dimensional nanosheets (high-bandgap domains) to 3D nanocrystals (low-bandgap domains). High-quality quasi-2D perovskite (PEA) 2 (FA) 3 Pb 4 Br 13 films are fabricated by solution engineering. Grazing-incidence wide-angle X-ray scattering measurements are conducted to study the crystal orientation, and transient absorption spectroscopy measurements are conducted to study the charge-carr...

In the fabrication of polymeric electroluminescent devices with indium-tin oxide (ITO) as anode, indium contamination of the polymers can greatly degrade the device performance. In the present study, we have used x-ray photoelectron spectroscopy to measure indium incorporation in poly(3,4-ethylene dioxythiophene):poly(styrene sulphonate), referred to as PEDOT:PSS, which were spincast on bare ITO and encapsulated ITO. We found that the deposition of a self-assembled monolayer of alkylsiloxanes on ITO prior to spincasting PEDOT:PSS was effective and practical in blocking the reactions between ITO and PEDOT:PSS.

The antioxidant activities of hot water extracts (HWECC) and ethanol extracts (EECC) from the dry bark of Cinnamomum cassia Presl were evaluated in this study. Results showed that at 1.0 mg/mL, the ethanol extracts of C. cassia (96.30%) exhibited a greater inhibition than the alpha-tocopherol (93.74%) on FeCl(2)-ascorbic acid induced lipid peroxidation of rat liver homogenate in vitro. From 0.05 to 1.0 mg/mL, the EECC demonstrated the highest superoxide anions scavenging activity and the strongest anti-superoxide formation activity (p < 0.05). The same extract also showed an excellent antioxidant activity in enzymatic and nonenzymatic liver tissue oxidative systems. EECC revealed the strongest antioxidant activity followed by alpha-tocopherol and HWECC. Compared to alpha-tocopherol, the IC(50) values of EECC were found to be lower in thiobarbituric acid test (IC(50) = 0.24 mg/mL vs 0.37 mg/mL), in cytochrome c test (IC(50) = 0.16 mg/mL vs 0.27 mg/mL) and in xanthine oxidase inhibition test (IC(50) = 0.09 mg/mL vs 0.19 mg/mL). The present study concludes that EECC could be used as a good source of antioxidant in the dietary supplement.

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