Doped Lead Halide White Phosphors for Very High Efficiency and Ultra‐High Color Rendering

Near‐UV‐pumped white‐light‐emitting diodes with ultra‐high color rendering and decreased blue‐light emission is highly desirable. However, discovering a single‐phase white light emitter with such characteristics remains challenging. Herein, we demonstrate that Mn doping as low as 0.027 % in the hybrid post‐perovskite type (TDMP)PbBr₄ (TDMP=trans‐2,5‐dimethylpiperaziniium) enables to achieve a bright pure white emission replicating the spectrum of the sun's rays. Thus, a white phosphor exhibiting an emission with CIE coordinates (0.330, 0.365), a high photoluminescence quantum yield of 60 % (new record for white light emission of hybrid lead halides), and an ultra‐high color rendering index (CRI=96, R9=91.8), corresponding to the record value for a single phase emitter was obtained. The investigation of the photoluminescence properties revealed how free excitons, self‐trapped excitons, and low amount of Mn dopants are coupled to give rise to such pure white emission.     

白光LED用Eu掺杂红色荧光粉

白光LED因亮度高、体积小、寿命长、高效节能、绿色环保等优点而引起人们的广泛关注,但是目前大部分白光LED用荧光粉的不足之处在于其发光效率较低,显色指数较差,色温较高,成本较高等等。红色荧光粉可明显改善白光LED的色温和显色指数,因此红色荧光粉在调制白光LED和改善其显色指数方面具有至关重要的作用。近年来红色荧光粉得到了深入研究,并有不少文献报道了新型的红色荧光粉。本文介绍了Eu~(3+)掺杂的线状红光发射荧光粉、Eu~(2+)掺杂的带状红光发射荧光粉并着重介绍了Eu~(2+)掺杂的新型窄带红光发射荧光粉,以及目前Eu掺杂红色荧光粉发展的不足及其改善方法。     

白光LED用Eu掺杂红色荧光粉

白光LED因亮度高、体积小、寿命长、高效节能、绿色环保等优点而引起人们的广泛关注,但是目前大部分白光LED用荧光粉的不足之处在于其发光效率较低,显色指数较差,色温较高,成本较高等等。红色荧光粉可明显改善白光LED的色温和显色指数,因此红色荧光粉在调制白光LED和改善其显色指数方面具有至关重要的作用。近年来红色荧光粉得到了深入研究,并有不少文献报道了新型的红色荧光粉。本文介绍了Eu³⁺掺杂的线状红光发射荧光粉、Eu²⁺掺杂的带状红光发射荧光粉并着重介绍了Eu²⁺掺杂的新型窄带红光发射荧光粉,以及目前Eu掺杂红色荧光粉发展的不足及其改善方法。     

Moisture‐Resistant Mn4+‐Doped Core–Shell‐Structured Fluoride Red Phosphor Exhibiting High Luminous Efficacy for Warm White Light‐Emitting Diodes

K₂TiF₆:Mn⁴⁺ is a highly efficient narrow‐band emission red phosphor with promising applications in white light‐emitting diodes (LEDs) and wide‐gamut displays. Nevertheless, the poor moisture‐resistant properties of this material hinder commercialization. A convenient reverse cation‐exchange strategy is introduced for constructing a core–shell‐structured K₂TiF₆:Mn⁴⁺@K₂TiF₆ phosphor. The outer K₂TiF₆ shell acts as a shield for preventing moisture in the air from hydrolyzing the internal MnF₆^2? group, while effectively cutting off the path of energy migration to surface defects, thereby increasing the emission efficiency (especially for the phosphors doped with high concentrations of Mn⁴⁺). Employed as a red phosphor, the packaged white LED exhibits an extraordinarily high luminous efficacy of 162 lm W^?1, a correlated color temperature (CCT) of 3510 K, and a color rendering index of 93 (R_a). Aging tests performed on this device at 85 °C and 85 % humidity for 480 h retain up to 89 % luminous efficacy. The findings could facilitate commercial application of K₂TiF₆:Mn⁴⁺@K₂TiF₆ phosphor.     

New Phosphors for White LEDs

White light-emitting diodes (WLEDs) have matched the emission efficiency of florescent lights and will rapidly spread as light source for homes and offices in the next 5 to 10 years. WLEDs provide a light element having a semiconductor light emitting layer (blue or UV LEDs) and photoluminescence phosphors. GaN-based highly efficient blue InGaN LEDs combined with phosphors can produce white light. These solid-state LED lamps have a number of advantages over conventional incandescent bulbs and halogen lamps, such as high efficiency to convert electrical energy into light, reliability, and long operating lifetime (about 100,000 hours). For the purpose of development of high energy-efficient white light sources, we need to produce highly efficient new phosphors, which can absorb excitation energy from blue or UV LEDs and generate emissions.In this paper, we investigate the development of blue or UV LEDs by the appropriate combination of new phosphors which can lead us to obtain high brightness white light. The criteria of choosing the best phosphors, for blue (380-450 nm) and UV (360-400 nm) LEDs, strongly depends on the absorption and emission of the phosphors. Moreover, the balance light between the light emission from blue LEDs and the yellow YAG:Ce,Gd phosphor is important to obtain white light with high color temperature. The phosphors with high efficiency which can be excited by UV LEDs are important to obtain the white light with high color rendering index.     

Colloidal Synthesis and Optical Properties of All‐Inorganic Low‐Dimensional Cesium Copper Halide Nanocrystals

Low‐dimensional metal halides have recently attracted extensive attention owing to their unique structure and photoelectric properties. Herein, we report the colloidal synthesis of all‐inorganic low‐dimensional cesium copper halide nanocrystals (NCs) by adopting a hot‐injection approach. Using the same reactants and ligands, but different reaction temperatures, both 1D CsCu₂I₃ nanorods and 0D Cs₃Cu₂I₅ NCs can be prepared. Density functional theory indicates that the reduced dimensionality in 1D CsCu₂I₃ compared to 0D Cs₃Cu₂I₅ makes the excitons more localized, which accounts for the strong emission of 0D Cs₃Cu₂I₅ NCs. Subsequent optical characterization reveals that the highly luminescent, strongly Stokes‐shifted broadband emission of 0D Cs₃Cu₂I₅ NCs arises from the self‐trapped excitons. Our findings not only present a method to control the synthesis of low‐dimensional cesium copper halide nanocrystals but also highlight the potential of 0D Cs₃Cu₂I₅ NCs in optoelectronics.     

Pressure-Tuned Multicolor Emission of 2D Lead Halide Perovskites with Ultrahigh Color Purity

The chemical diversity and structural flexibility of lead halide perovskites (LHPs) offer tremendous opportunities to tune their optical properties through internal molecular engineering and external stimuli. Herein, we report the wide-range and ultrapure photoluminescence emissions in a family of homologous 2D LHPs, [MeOPEA]₂PbBr_4−4xI_4x (MeOPEA=4-methoxyphenethylammonium; x=0, 0.2, 0.425, 0.575, 1) enabled through internal chemical pressure and external hydrostatic pressure. The chemical pressure, induced by the C−H⋅⋅⋅π interactions and halogen doping/substitution strengthens the structural rigidity to give sustained narrow emissions, and regulates the emission energy, respectively. Further manipulation of physical pressure leads to wide-range emission tuning from 412 to 647 nm in a continuous and reversible manner. This work could open up new pathways for developing 2D LHP emitters with ultra-wide color gamut and high color purity which are highly useful for pressure sensing.     

Metal‐Free Triplet Phosphors with High Emission Efficiency and High Tunability

Design of highly efficient phosphorescent emitters based on metal‐ and heavy atom‐free boron compounds has been demonstrated by taking advantage of the singlet fission process. The combination of a suitable molecular scaffold and appropriate electronic nature of the substituents has been utilized to tailor the phosphorescence emission properties in solution, neat solid, and in doped PMMA thin films.     

Simultaneous Long‐Persistent Blue Luminescence and High Quantum Yield within 2D Organic–Metal Halide Perovskite Micro/Nanosheets

Molecular solid‐state materials with long‐lived luminescence (such as thermally activated delayed fluorescence (TADF) and room temperature phosphorescence (RTP) systems) are promising for display, sensoring, and bio‐imaging applications. However, the design of such materials that exhibit both long luminescent lifetime and high solid‐state emissive efficiency remains an open challenge. Two‐dimensional (2D) organic–metal halide perovskite materials have a high blue‐emitting quantum yield of up to 63.55 % and ultralong TADF lifetime of 103.12 ms at ambient temperature and atmosphere. Our design leverages the combined influences of a 2D space/electronic confinement effect and a modest heavy‐atom tuning strategy. Photophysical studies and calculations reveal that the enhanced quantum yield is due to the rigid laminate structure of perovskites, which can effectively inhibit the non‐radiative decay of excitons.     

Cesium Lead Halide Perovskite Nanostructures: Tunable Morphology and Halide Composition

Inorganic halide perovskite (CsPbX₃) nanostructures have gained considerable interest in recent years owing to their enhanced stability and optoelectronic applications. Recent developments in the synthesis of nanostructures are reviewed. The impact of the precursor and ligand nature, temperature and growth time on the morphology and shape tuning of CsPbX₃ nanostructures is described in relation to their optical properties. The presynthetic and postsynthetic anion exchange strategies to retain pre‐existing crystal phase and shape are discussed in this minireview.     

Sm掺杂的红色荧光粉的制备及发光性能研究

采用高温固相法合成了Ca3Gd2WO9/xSm3＋系列红色荧光材料。研究了合成样品的最佳烧结温度和时间分别为1 100℃和3 h,讨论了Sm3＋的掺杂浓度对Ca3Gd2WO9/x Sm3＋发光强度的影响,当x为1.0%（摩尔分数）时,样品的相对发光强度达到最大值。测量了荧光粉的X射线衍射谱和荧光光谱。结果表明,该样品能够被434 nm的可见光有效激发,主发射峰位593 nm附近,对应于Sm3＋的4G5/2→6H7/2跃迁,可作为白光发光LED的红色发光材料。     

Lead Halide Perovskite Quantum Dots To Enhance the Power Conversion Efficiency of Organic Solar Cells

The facile synthesis, solution‐processability, and outstanding optoelectronic properties of emerging colloidal lead halide perovskite quantum dots (LHP QDs) makes them ideal candidates for scalable and inexpensive optoelectronic applications, including photovoltaic (PV) devices. The first demonstration of integrating CsPbI₃ QDs into a conventional organic solar cell (OSC) involves embedding the LHP QDs in a donor–acceptor (PTB7‐Th:PC₇₁BM) bulk heterojunction. Optimizing the loading amount at 3 wt %, we demonstrate a power conversion efficiency of 10.8 %, which is a 35 % increase over control devices, and is a record amongst hybrid ternary OSCs. Detailed investigation into the mechanisms behind the performance enhancement shows that increased light absorption is not a factor, but that increased exciton separation in the acceptor phase and reduced recombination are responsible.     

白光电致发光二极管用发光材料研究进展

白光电致发光二极管(LED)是固体照明的重要光源.荧光体转换是获取白光LED的主要途径之一.当前,转换用荧光体的研究在发光材料领域中最活跃.本文对近年来白光LED用发光材料新体系的研究进展作了评述.     

铅卤钙钛矿-聚合物复合材料的制备及应用

铅卤钙钛矿纳米晶具有优异的光电性能,在太阳能电池、光电探测和生物成像等领域展现出巨大的发展潜力.然而,铅卤钙钛矿纳米晶自身稳定性差的缺陷制约了其在实际生活中的应用.将铅卤钙钛矿纳米晶嵌入到聚合物中以制备钙钛矿-聚合物复合材料是近年来发展起来的一种有效增强钙钛矿稳定性的策略,特别是致密的聚合物基质赋予钙钛矿纳米晶优异的水...     

Manganese‐Doped Highly Ordered Mesoporous Silicate with High Efficiency for Oxidation Suppression

Herein, we demonstrate a facile approach to manganese‐doped highly ordered mesoporous silicate with oxidation‐suppression function. As biocompatible supports of guest ions, the ordered mesoporous silicate was synthesized by evaporation‐induced self‐assembly. The phase‐transition from disordered to lamellar structures in the highly ordered mesoporous structure of these porosity‐tuned materials was controlled by adjusting the concentration of a lab‐made polystyrene‐b‐polyethylene oxide copolymer. Manganese was successfully incorporated as a guest in the hexagonally packed mesoporous silicate by using an ultrasound‐assisted technique. The incorporation of manganese ions into the pores of a mesoporous silicate support could be induced for host–guest functional applications. Manganese‐doped mesoporous silicate structures have been examined for their use as antioxidizing agents by electron spin resonance (ESR) measurements and radical‐scavenging tests. The manganese atoms in the mesoporous structures could act in a free‐radical‐scavenging capacity, much like manganese nanoparticles. The high efficiency of their oxidation‐suppression function is extended for application to catalytic products.     

紫外光发光二极管用铋与铕离子掺杂的氧化钇红光荧光体研究

将铋离子（Bi^3＋）加入铕离子掺杂的氧化钇红色荧光体中, 探讨了其结构与光学性质. 发现加入铋离子能促进红色荧光体于300～380 nm的紫外线能量吸收, 此乃由于铋离子吸收紫外线能量再以能量转移的方式传给铕离子.     

激光作用铅卤钙钛矿的机理与应用

近年来,铅卤钙钛矿纳米晶因其易制备,低成本,高性能等特性引起了人们极大的关注。钙钛矿纳米晶的光电性能优越应用潜力巨大,然而稳定性问题制约着它进一步发展,使其无法与已经商业化的应用相匹敌。针对钙钛矿材料的稳定性问题,人们展开了很多研究,其中一个方面就是光照稳定性。该方面的研究可以为制备高稳定性钙钛矿材料和器件奠定基础,还可以利用光照(特别是激光)来调控钙钛矿的结构和性能,拓展其在光电领域的全方位应用。本文专注于激光照射下钙钛矿的变化及其相关应用,首先综述了激光辐照铅卤钙钛矿时出现的变化现象以及微观机理;其次,基于这些变化机理,介绍了最近研究人员如何使用激光技术对钙钛矿薄膜和器件进行性能调控,以及激光直写钙钛矿技术的相关应用。     

Size- and Halide-Dependent Auger Recombination in Lead Halide Perovskite Nanocrystals

Lead halide perovskite nanocrystals (NCs) hold strong promise for a variety of light-harvesting, emitting, and detecting applications, all of which, however, could be complicated by multicarrier Auger recombination. Therefore, complete documentation of the size- and composition-dependent Auger recombination rates of these NCs is highly desirable, as it can guide system design in many applications. Herein we report the synthesis and Auger measurements of monodisperse APbX₃ (A=Cs and FA; X=Cl, Br, and I) NCs in an extensive size range (ca. 3–9 nm). The biexciton Auger lifetime of all the NCs scales linearly with the NC volume. The scaling coefficient is virtually independent of the cation but rather depends sensitively on the anion, and is 0.035, 0.085, and 0.142 ps nm⁻³ for Cl, Br, and I, respectively. In all of these nanocrystals the Auger recombination is much faster than in standard CdSe and PbSe NCs (ca. 1 ps nm⁻³).     

Pressure‐Induced Emission Enhancement,Band‐Gap Narrowing,and Metallization of Halide Perovskite Cs3Bi2I9

Low‐toxicity, air‐stable bismuth‐based perovskite materials are attractive substitutes for lead halide perovskites in photovoltaic and optoelectronic devices. The structural, optical, and electrical property changes of zero‐dimensional perovskite Cs₃Bi₂I₉ resulting from lattice compression is presented. An emission enhancement under mild pressure is attributed to the increase in exciton binding energy. Unprecedented band gap narrowing originated from Bi−I bond contraction, and the decrease in bridging Bi‐I‐Bi angle enhances metal halide orbital overlap, thereby breaking through the Shockley–Queisser limit under relatively low pressure. Pressure‐induced structural evolutions correlate well with changes in optical properties, and the changes are reversible upon decompression. Considerable resistance reduction implies a semiconductor‐to‐conductor transition at ca. 28 GPa, and the final confirmed metallic character by electrical experiments indicates a wholly new electronic property.