脂质体封端CsPbX3(X=Cl,Br,I)纳米晶体的制备及在发光二极管中的应用

以脂质体充当表面封端配体修饰合成后的CsPbX₃纳米晶体.封端CsPbX₃纳米晶能保持原始形状和粒径大小,相对量子产率提升至（100±3）%,发射光谱在411~626 nm范围内可调.将其存储于空气（温度25℃,相对湿度50%）中150 d仍保持立方晶型.以DOPC-CsPbBr₃为颜色转换器可制造显色指数高达91.2的白色发光二极管,应用前景广阔.     

多色高发光效率CsPbX3(X=Cl,Br,I)钙钛矿量子点的制备及其在发光二极管中的应用

采用室温合成法制备出一系列具有高发光效率和多色发光的CsPbX₃钙钛矿量子点(PQDs),反应全过程快速简便,且通过调节不同的卤素组成(Cl,Br,I)可以实现CsPbX₃ PQD的多色发光。 通过表征证明,CsPbX₃ PQDs呈立方晶型,平均粒径约为10 nm,发射光谱覆盖可见光波长范围为410~630 nm,半峰宽14~38 nm,荧光量子产率10%~90%。 最后将CsPbX₃ PQDs应用于发光二极管(LED)器件的制备中,在恒定电压下工作时,能保持LED器件的发光颜色、强度和颜色坐标不变。     

多维CsPbX3无机钙钛矿材料的制备及其在太阳能电池中的应用

近年来全无机CsPbX3(X=Cl、Br、I)型钙钛矿材料由于其高吸光系数、低激子束缚能、长的载流子扩散长度等优点使其在太阳能电池(PSC)器件应用方面备受关注.高效的合成方法和精准的形貌控制对无机钙钛矿的光学性质及其太阳能电池光电性能及稳定性至关重要.本文系统介绍了不同维度无机钙钛矿材料包括零维量子点、一维纳米线/棒...     

无机铅卤钙钛矿纳米晶的合成、性能及应用

无机铅卤钙钛矿CsPbX₃(X=Cl,Br,I)纳米晶因具有较高荧光量子效率(~90%)、发光波长覆盖整个可见光谱(400~700 nm)、半高宽相对较窄(12~42 nm)等诸多优点而备受关注,这些性能使之成为当前最具有潜在应用价值的发光材料之一。 因此,近年来对该类无机铅卤钙钛矿材料的报道越来越多。 本文主要介绍了无机铅卤钙钛矿发光材料的发展历程、结构、制备方法、生长机理及当前的主要应用领域等,最后概括了无机铅卤钙钛矿发光材料在当前研究背景下所面临的问题并展望了下一阶段的发展方向,为进一步提高其光学性能及开发新型高效的无机铅卤钙钛矿发光材料奠定基础。     

Ag(PPh3)nX(n=1,2,3；X=Cl,Br,I)的电化学合成

银配合物;;三苯基膦;电合成;Ag(PPh3)nX(n=1;2;3；X=Cl;Br;I)的电化学合成     

磁性Fe3O4纳米晶制备及应用

磁性Fe₃O₄纳米晶由于其独特的磁性能,已在许多领域得到了广泛的应用,并且在不同的应用领域其制备方法也不尽相同。本文综述了近年来磁性Fe₃O₄纳米晶的液相制备方法,如沉淀法、溶剂热法、溶胶-凝胶法、微乳液法、微波超声法等研究进展,对这些制备方法的特点进行了归纳概括,并详细分析了制备工艺中不同影响因素对Fe₃O₄纳米晶结构与性能的影响。同时,对磁性Fe₃O₄纳米晶在磁流体、微波吸收、污水处理、催化、药物载体、生物酶固定、生物传感器等方面的应用及发展趋势进行了评述,以期对Fe₃O₄纳米晶的制备及应用有较全面的认识。     

球形La2O3∶Eu纳米晶的制备及其发光特性

近年来纳米材料的发展及纳米材料所具有的特异的光学性质,使得纳米发光材料引起越来越多的关注。La2O3结构简单,易于合成,价格便宜．因此以La2O3为基质的发光材料已有很多报道。Mekittric等研究认为,发光材料的形貌,如颗粒度、形状、结晶性等．是影响发光效率的一个重要因素．球形颗粒可以提高其密堆性．从而能有效地提高产品的发光亮度。     

Ag@AgX(X=Cl,Br,I)及其复合物光催化剂的研究进展

综述了具有表面等离子体共振效应的光催化剂Ag@AgX(X=Cl,Br,I)及其与TiO2、BiOX、BiVO4、ZnO等复合物的光催化机理、应用等方面的进展,并展望了Ag@AgX(X=Cl,Br,I)及其复合物未来的发展方向和研究内容。     

纳米晶La_（1－_x）Sr_xFeO_3的合成及气敏特性的研究

用柠檬酸盐法合成出Ｌａ_（１－_ｘ）Ｓｒ_ｘＦｅＯ_３（ｘ＝０．１，０．２，０．３，０．４）原粉，再经固相反应得到纳米晶粉末，用ＴＧ、ＤＴＡ、ＸＲＤ、ＩＲ进行了表征，确证复合氧化物Ｌａ_（１－_ｘ）Ｓｒ_ｘＦｅＯ_３为钙钛矿型结构，粒径在１０～２５ｎｍ之间。实验结果表明，随着固相反应条件不同，产物粒径呈规律性变化．气敏特性研究表明，该纳米晶材料对乙醇有较高的选择性和灵敏度，其选择性顺序为Ｌａ_（０．９）Ｓｒ_（０．１）ＦｅＯ_３＞ＬａＦｅＯ_３＞ＬａＦｅＯ_３（大晶粒）。     

聚合物裂解法制备稀土铁氧体LnFeO_3(Ln=Pr,Sm,Eu,Gd)纳米晶

以丙烯酸和稀土离子为原料,经原位聚合裂解法合成聚合物前驱体[1Ln(Ln=Pr,Sm,Eu,Gd)];1Ln在空气氛中于500℃热解3 h制得4个稀土铁氧体纳米晶[Ln Fe O3(2Pr~2Gd)],其结构和形貌经FT-IR,TGA,XRD和SEM确证。     

Near‐Unity Photoluminescence Quantum Efficiency for All CsPbX3 (X=Cl,Br, and I) Perovskite Nanocrystals: A Generic Synthesis Approach

In a generic synthesis approach, all three CsPbX₃ (X=Cl, Br and I) perovskite nanocrystals having near unity quantum yields is reported. This has been achieved by injecting the desired amount of preformed alkylammonium halide salts which acted as a dual source providing halide ions and the capping agent to an equimolar amount of non‐halide Pb and Cs precursors in a reaction flask at an optimized reaction temperature. The composition sensitivity of Pb to Cs ratio, high temperature reaction, and injection of ammonium halide remained the key parameters for obtaining the high quantum yields. Details of the reaction process, use of different reagents and setting up the reaction parameters are reported.     

Luminescent Thin Films Enabled by CsPbX3 (X=Cl,Br, I) Precursor Solution

Inorganic cesium lead halide perovskite nanocrystals are candidates for lighting and display materials due to their outstanding optoelectronic properties. However, the dissolution issue of perovskite nanocrystals in polar solvents remains a challenge for practical applications. Herein, we present a newly designed one-step spin-coating strategy to prepare a novel multicolor-tunable CsPbX₃ (X=Cl, Br, I) nanocrystal film, where the CsPbX₃ precursor solution was formed by dissolving PbO, Cs₂CO₃, and CH₃NH₃X into the ionic liquid n-butylammonium butyrate. The as-designed CsPbX₃ nanocrystal films show high color purity with a narrow emission width. Also, the blue CsPb(Cl/Br)₃ film demonstrates an absolute photoluminescence quantum yields (PLQY) of 15.6 %, which is higher than 11.7 % of green CsPbBr₃ and 8.3 % of red CsPb(Br/I)₃ film. This study develops an effective approach to preparing CsPbX₃ nanocrystal thin films, opening a new avenue to design perovskite nanocrystals-based devices for lighting and display applications.     

Near‐Unity Photoluminescence Quantum Efficiency for All CsPbX3 (X=Cl,Br, and I) Perovskite Nanocrystals: A Generic Synthesis Approach

In a generic synthesis approach, all three CsPbX₃ (X=Cl, Br and I) perovskite nanocrystals having near unity quantum yields is reported. This has been achieved by injecting the desired amount of preformed alkylammonium halide salts which acted as a dual source providing halide ions and the capping agent to an equimolar amount of non‐halide Pb and Cs precursors in a reaction flask at an optimized reaction temperature. The composition sensitivity of Pb to Cs ratio, high temperature reaction, and injection of ammonium halide remained the key parameters for obtaining the high quantum yields. Details of the reaction process, use of different reagents and setting up the reaction parameters are reported.     

Composition‐Dependent Hot Carrier Relaxation Dynamics in Cesium Lead Halide (CsPbX3, X=Br and I) Perovskite Nanocrystals

Cesium‐based perovskite nanocrystals (NCs) have outstanding photophysical properties improving the performances of lighting devices. Fundamental studies on excitonic properties and hot‐carrier dynamics in perovskite NCs further suggest that these materials show higher efficiencies compared to the bulk form of perovskites. However, the relaxation rates and pathways of hot‐carriers are still being elucidated. By using ultrafast transient spectroscopy and calculating electronic band structures, we investigated the dependence of halide in Cs‐based perovskite (CsPbX₃ with X=Br, I, or their mixtures) NCs on the hot‐carrier relaxation processes. All samples exhibit ultrafast (<0.6 ps) hot‐carrier relaxation dynamics with following order: CsPbBr₃ (310 fs)>CsPbBr_1.5I_1.5 (380 fs)>CsPbI₃ NC (580 fs). These result accounts for a reduced light emission efficiency of CsPbI₃ NC compared to CsPbBr₃ NC.     

Synthesis,Crystal Structure,and Optical Properties of (CH3NH3)2CoX4 (X = Cl,Br, I,Cl0.5Br0.5, Cl0.5I0.5, Br0.5I0.5)

The reaction of methylammonium halides and cobalt halides yielded the organic‐inorganic hybrid compounds of general formula (CH₃NH₃)₂CoX₄. By varying the different halides, we were able to synthesize the whole row from Cl to I as well as some mixed halides compounds and to determinate the crystal structures. (CH₃NH₃)₂CoX₄ (X = Cl, Br, Cl_0.5Br_0.5, Br_0.5I_0.5) crystallize isotypic to (CH₃NH₃)₂HgCl₄ in space group P2₁/c with Z = 4 [X = Cl: a = 7.6483(9), b = 12.6885(18), c = 10.8752(12) Å, β = 96.639(9)°; X = Cl_0.5Br_0.5: a = 7.8271(9), b = 12.9543(9), c = 11.1007(11) Å, β = 96.320(8)°; X = Br: a = 7.9782(2), b = 13.1673(2), c = 11.2602(2) Å, β = 96.3260(10)° and X = Br_0.5I_0.5: a = 8.2435(12), b = 13.645(2), c = 11.5856(18) Å, β = 95.54(2)°]. The mixed halides show a statistic distribution in both cases. In (CH₃NH₃)₂CoCl₂I₂ an ordered variant is realized representing a new structure type [C2/m, Z = 4, a = 18.808(4), b = 7.3604(7), c = 10.4109(17) Å, β = 120.364(13)°]. (CH₃NH₃)₂CoI₄ crystallizes again isotypic to the respective mercury compound [(CH₃NH₃)₂HgCl₄] [Pbca, Z = 8, a = 10.9265(5), b = 12.1552(5), c = 20.9588(9) Å]. All structures are build up by inorganic tetrahedral [CoX₄]^2– anions and organic (CH₃NH₄)⁺ cations. Additionally the Raman spectra as well as the optical reflectance spectra are discussed.