Happiness, Life satisfaction, Relative deprivation, Inequality, Income, Transition economies, Market economy,

light with the emission wavelength of 620-640 nm is an essential part for highdefinition display; however, compared with the green-counterpart, the electroluminescence (EL) performance of the colorsaturated red and blue perovskite emitters is much poorer. Ever since the first red-PeLED with an EL peak at 630 nm was demonstrated by Friend and coworkers, [1] efforts have been paid to improve the emitter photoluminescence quantum yield (PL QY) toward high-performing devices. Tan and coworkers applied a trimethylaluminum vapor-based crosslinking method to increase the PL QY of CsPb(Br/I) 3 nanocrystals (NCs) and gave rise to an EQE of 1.4%. [28] Brighter emitters leading to more efficient LEDs have been also observed in perovskite NCs of other colors and components, and strategies including doping, [29][30][31][32][33][34] surface capping, [35][36][37][38][39][40][41] core-shell structures, [42,43] and anion-exchange [25,[44][45][46][47] have been employed. For lead-halide perovskites, most charge recombination centers are localized on the crystal surfaces, and lead atoms who may cause strong exciton quenching are facile to form. [35,[38][39][40] Thus, the PL QY of red CsPb(Br/I) 3 NCs can increase through reducing the number of surface lead atoms. Aside from the excellent optical properties, the electric conductivity of perovskite NCs is another crucial factor for the performance of perovskite electroluminescent devices. Metal doping has been considered as a promising avenue to control over the electronic and optical performance of perovskite NCs. However, the limited improvement of metal doped CsPb(Br/I) 3 PeLEDs indicates that new methods are necessary. [32] Furthermore, doping perovskite with transition metal ions (Cu 2+ , Ni 2+ , Zn 2+ ) broadened the emission bands, and incorporation of Mn 2+ or lanthanide ions introduced new emission centers in perovskite NCs, leading to poor color purity of PeLEDs. [31,33,34] Here, benzyl iodide (BI) was chosen to passivate the CsPb(Br/I) 3 NC surface where the iodide can bond to the surface Pb atoms leading to reduced non-recombination centers. Interestingly, we found that the electrons tend to transfer from CsPb(Br/I) 3 NC to the surface electron acceptor-aromatic rings, leading to p-doping of the CsPb(Br/I) 3 NCs, thus allowing us to control over the energy levels and electrical conductivity. With the help of BI, the NC PL QY is greatly increased Color-saturated red light-emitting diodes (LEDs) with emission wavelengths at around 620-640 nm are an essential part of high-definition displays. Metal halide perovskites with very narrow emission linewidth are promising emitters, and rapid progress has been made in perovskite-based LEDs (PeLEDs); however, the efficiency of the current color-pure red PeLEDs-still far lags behind those of other-colored ones. Here, a simple but efficient strategy is reported to gradually down-shift the Fermi level of perovskite nanocrystals (NCs) by controlling the interaction between NCs and their surface molecular electron acceptor-benzyl iodide ...

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Nickel oxide (NiO x ) is a promising hole-transporting material for perovskite light-emitting diodes (PeLEDs) because of its low cost, excellent stability, and simple fabrication process. However, the electroluminescence efficiencies of NiO x -based PeLEDs are greatly limited by inefficient hole injection and exciton quenching at the NiO x –perovskite interfaces. Here, a novel interfacial engineering method with sodium dodecyl sulfate-oxygen plasma (SDS-OP) is demonstrated to simultaneously overcome the aforementioned issues. Experimental results reveal that a short OP treatment on the top of the SDS-coated NiO x significantly deepens the NiO x work function (from 4.23 to 4.85 eV) because of the formation of a large surface dipole, allowing for efficient hole injection. Moreover, the SDS-OP layer passivates the electronic surface trap states of perovskite films and suppresses the exciton quenching by NiO x . These improvements inhibit the nonradiative decays at the NiO x –perovskite interface. As a result, the external quantum efficiency of CsPbBr3 LEDs is increased from 0.052 to 2.5%; that of FAPbBr3 nanocrystals LEDs is increased from 5.6 to 7.6%.

Although the positive associations between social capital, household income and life satisfaction are well documented, little is known about how income actually shapes the relation between structural social capital and life satisfaction. This study investigates the roles of economic condition in determining the relationships between life satisfaction and three aspects of structural social capital, namely network size, neighborhood interaction and social participation. This study uses a random sample of 6002 adults nested in 2365 families from three regions in China: Beijing, Shanghai and Guangdong-province and applies multilevel linear regression models. The results firstly show that household income and structural social capital are positively associated with life satisfaction. Further analyses on the interaction effects find that household income substantively reduces the association between a social network size and life satisfaction but increases the relationship between social participation and life satisfaction. In addition, the differences between families explain about 25 % unexplained variances of life satisfaction.