杂化钙钛矿(NH3C6H12NH3)CuCl4的制备与表征

采用低温溶液法合成了含有二铵阳离子结构的新型二维层状结构的有机/无机杂化钙钛矿材料（NH₃C₆H₁₂NH₃） CuCl₄。采用元素分析、红外光谱、X射线衍射和紫外-可见光吸收光谱等手段对其结构与性能进行了表征。结果表明该材料的紫外-可见吸收光谱吸收峰位于285 nm和387 nm,层间距为1.18 nm。二铵阳离子的引入,使有机层⁺NH₃C₆H₁₂NH₃+与2个相邻的无机框架CuCl₄^2-分别通过较强的氢键结合在一起,排列更为规整,热稳定性更高。与单铵阳离子结构的杂化钙钛矿材料相比,由于不存在两层有机分子层间较弱的范德华力,（NH₃C₆H₁₂NH₃） CuCl₄材料的电阻率为1.36×10⁵ Ω·cm,比单胺结构的杂化钙钛矿材料的电阻率低3个数量级。     

层状有机-无机杂化钙钛矿(C7H12N2)PbBr4的合成、结构及发光性质

通过向杂化体系中引入特殊的有机配体2-（2-氨基乙基）吡啶,利用溶液冷却技术,合成了一种二维层状有机-无机杂化钙钛矿结构材料的化合物(C7H12N2)PbBr4的晶体。 X射线单晶衍射结果表明,化合物(C7H12N2)PbBr4的单晶结构属于正交晶系,Pbca空间群,a=1.702 3 nm,b=0.828 9 nm,c=2.022 4 nm,Z=8。 无机部分是由共顶点的PbBr6金属卤化物八面体组成的二维平面片层。 采用了相对扭曲构型的有机胺阳离子与二维无机片层通过氢键作用组成了杂化钙钛矿结构。 对其光学性质进行了测试。荧光光谱的特征发射峰出现在422 nm处。     

一个各向异性磁稀释杂化钙钛矿系列[CH_3NH_3][Co_x Zn_(1-x)(HCOO)_3]（英文）

作为与传统纯无机钙钛矿材料互补的体系,有机-无机或杂化钙钛矿材料结合了有机和无机成分各自的特性,在相变、临界现象和相关功能性质的研究中展现了众多新的可能性和机会。其中,金属甲酸铵钙钛矿表现优越,且其功能和性质十分依赖于金属离子和铵的特性。本工作借助固体化学中的固溶体策略,研究各向异性磁稀释杂化钙钛矿[CH_3NH_3][Co_(x )Zn_(1-x)(HCOO)_3]系列的制备、结构和磁性。该系列的全程固溶体(x=0–1或摩尔百分比Co%=0–100%)都可以用溶液化学方法制备获得,并由单晶和粉末X射线衍射确定了固溶体全程同构。它们都属于正交晶系,空间群Pnma,晶胞参数范围为a=8.3015(2)–8.3207(3)?,b=11.6574(4)–11.6811(5)?,c=8.1315(3)–8.1427(4)?,V=787.89(5)–790.98(7)?~3(1?=0.1 nm)。钙钛矿结构由金属-甲酸的简单立方阴离子骨架和骨架孔穴中的CH_3NH_3~+阳离子构成,CH_3NH_3~+阳离子和骨架之间形成N―H···O氢键。在这个系列中,固溶体晶体结构的点阵和结构参数几乎没有变化。因此,该系列提供了一个很好的在结构和分子几何参数不变的条件下研究磁稀释效应的分子磁性体系。在逐步稀释的过程中,Co~(2+)离子的磁各向异性和逐渐消失的较大自旋倾斜的贡献,抑制或减少了在低温和低场下的磁化强度,这与各向同性[CH_3NH_3][Mn_(x )Zn_(1-x)(HCOO)_3]体系在磁稀释时磁化强度增大的行为相反。实验获得的逾渗阈值为(Co%)_P=27(1)%(或x _P=0.27(1)),低于按逾渗理论得到的简单立方格子上的逾渗阈值31%,这也是由于[CH_3NH_3][Co_(x )Zn_(1-x)(HCOO)_3]体系磁各向异性的缘故。此外,观察到纯金属Co和Zn成员在约120 K左右发生少见的非公度相变。低温下的非公度性对于磁性质也产生一定的影响。     

有机/无机杂化钙钛矿(C14H13N2O2)2PbCl4的制备与表征

合成了一种新颖的有机/无机杂化钙钛矿(C14H13N2O2)2PbCl4材料,采用元素分析、红外光谱(FT-IR)、紫外可见吸收光谱(UV-Vis)、透射电镜(TEM)、电子衍射(ED)、紫外可见光声光谱(UV-Vis PAS)和表面光电压谱(SPS)等手段对其分子结构和聚集态、光学性质和光、电特性进行了表征。结果表明,这种材料具有较好的有序性,在紫外光波段同时具有较好的光电响应和光声特性。     

一种基于碘化铅的有机/无机杂化钙钛矿材料传输性能的研究

合成了一种新型的有机/无机杂化钙钛矿(NH3C6H4OC6H4NH3)PbI4, 采用元素分析、紫外-可见光吸收光谱、X射线衍射和透射电镜对其结构进行了表征, 结果表明这种材料具有规则的层状结构, 有序性高. 对这种材料的薄膜进行了伏安测试, 结果表明该材料属于n型半导体, 其电子迁移率达到0.065 cm2•V－1•s－1, 在光电器件领域有着潜在的应用前景.     

紫外光辐照下CH3NH3PbI3基钙钛矿太阳能电池失效机制

随着光伏产业的不断发展,有机无机杂化钙钛矿太阳能电池的研发成为科学与工业界广泛关注的焦点。到目前为止,其光电转换效率已经提高到了25.2%,成为替代硅基太阳能电池的核心方案之一。然而,钙钛矿太阳能电池的稳定性较差,容易受到环境中氧气、水分、温度甚至光照的影响,这严重制约了其大规模推广与应用。大量科学研究表明,如何避免紫外辐照下有机无机杂化钙钛矿太阳能电池的性能衰减,对于提高钙钛矿太阳能电池的光照稳定性至关重要。然而到目前为止,仍然没有系统的工作来对紫外辐照下钙钛矿太阳能电池性能以及微结构演化过程进行详细的表征与分析。本文中,我们利用聚焦离子束-扫描电子显微分析(FIB-SEM)以及球差校正透射电子显微分析(TEM)等技术,全面地研究了紫外辐照过程中有机无机杂化钙钛矿太阳能电池性能变化规律以及电池微结构演化特征。实验结果表明,紫外辐照过程中太阳能电池内部会形成0.5–0.6 V的内建电场,钙钛矿中的I^-离子在电场的驱动下向金属Au电极和空穴传输层2, 2’, 7, 7’-四[N, N-二(4-甲氧基苯基)氨基]-9, 9'-螺二芴(Spiro-OMeTAD)一侧迁移;随后,空穴传输层与金电极的界面处,碘离子与光生空穴一起与金电极发生反应,将金属态Au氧化成离子态Au⁺。而Au⁺离子则在内建电场的驱动下反向迁移穿过钙钛矿MAPbI₃层,直接被SnO₂和MAPbI₃界面处的电子还原形成金属Au纳米团簇。除此之外,紫外辐照过程中钙钛矿太阳能电池性能降低的同时,往往伴随着Spiro-OMeTAD与钙钛矿界面处物质迁移、钙钛矿薄膜内晶界展宽以及Au纳米颗粒周围MAPbI₃物相分解等现象。以上各种因素的协同作用,共同导致了紫外光照下有机无机杂化钙钛矿太阳能电池光电转换性能(PCE)、开路电压(V_oc)以及短路电流(J_sc)等性能参数的急剧下降。     

杂化钙钛矿光伏材料的合成及热稳定性研究——推荐一个综合化学实验

介绍了一个综合性化学实验,内容包括一步溶液法制备有机-无机杂化钙钛矿光伏材料、材料结构与形貌表征、吸光系数测定及热稳定性研究。     

以钴-哒嗪阳离子为模板构筑的多酸基有机-无机杂化材料

利用水热方法合成了一种Keggin型多酸基有机无机杂化材料,化学式为(Hpydz)Na[Co(pydz)_4(H_2O)_2][SiW_(12)O_(40)]·3H_2O(pydz=pyridazine).单晶X-射线研究表明,在该化合物中,Keggin型多阴离子与钠离子连接构筑成三维孔状结构,其中钴-哒嗪阳离子有机基团作为客体分子,通过静电相互作用存在于三维孔道结构中,构筑成有机-无机杂化材料.该化合物属于单斜晶系,空间群为C_2/c,晶胞参数a=1.937 7(2)nm,b=1.678 8(2)nm,c=1.768 0(2)nm,α=90°,β=98.612(3)°,γ=90°,V=5.686 51nm~3.     

基于有机/无机杂化钙钛矿有序结构的异质结及其光伏性能的研究

研究了一种新型的有机/无机杂化钙钛矿材料(3-BrC₃H₆NH₃)₂CuBr₄薄膜的聚集态形貌和良好的微观有序性特征, 霍尔迁移率测试结果表明该材料为p型半导体, 空穴迁移率为0.0025 cm²•V^－1•s^－1. 利用其在紫外-可见光谱范围内与C₆₀薄膜具有良好的光吸收互补性, 制备并研究了(3-BrC₃H₆NH₃)₂CuBr₄/C₆₀层状异质结结构中的暗态传输和光伏性能. 对不同退火温度下杂化钙钛矿薄膜的聚集态特性和器件性能之间的联系进行了探讨, 结果表明在低温退火条件下, 由于钙钛矿结构材料中有机组分排列更加有序, 器件显示更好的性能.     

可溶液加工的有机-无机杂化钙钛矿:超越光伏应用的“梦幻”材料

有机-无机杂化钙钛矿材料是可通过溶液工艺低温制备得到的直接带隙半导体晶体薄膜.在众多可溶液加工的半导体材料中,有机-无机杂化钙钛矿薄膜是为数不多的低缺陷密度、双极子传输性能优异的晶体薄膜,同时兼具宽光谱吸收和长载流子扩散距离等特性,是平面异质结太阳能电池的理想选择.另外,作为低缺陷密度的直接带隙半导体晶体材料,杂化钙钛矿薄膜具有优异的发光特性.其发光波长可通过能带工程(在分子水平上改变其组分)进行调节,因此有望在发光二极管和激光等光电器件中得到新应用.总结了钙钛矿材料的优异特性和目前应用研究的进展,并对其未来发展做了展望.     

Luminescence properties of efficient X-ray phosphors of YBa3B9O18, LuBa3(BO3)3, α-YBa3(BO3)3 and LuBO3

The samples of YBa₃B₉O₁₈, LuBa₃(BO₃)₃, α-YBa₃(BO₃)₃ and LuBO₃ powders have been synthesized by the solid-state reaction methods at high temperature and their X-ray excited luminescent properties were investigated. All the studied materials show a broad emission band in the wavelength range of 300-550 nm with the peak centers at about 385 nm for YBa₃B₉O₁₈ and LuBa₃(BO₃)₃, 415 nm for α-YBa₃(BO₃)₃ and 360 nm for LuBO₃ powders, respectively. Even though those compounds have the different atomic structures, they have the common structural feature of each yttrium or lutetium ion bonded to six separate BO₃ groups, i.e., octahedral RE(BO₃)₆ (RE=Lu or Y) moiety. This octahedral RE(BO₃)₆(RE=Lu or Y) moiety seems to be an important structural element for efficient X-ray excited luminescence of those compounds, as are the edge-sharing octahedral TaO₆ chains for tantalate emission.     

Non-centrosymmetric Ba3Ti3O6(BO3)2

The compound previously reported as Ba₂Ti₂B₂O₉ has been reformulated as Ba₃Ti₃B₂O₁₂, or Ba₃Ti₃O₆(BO₃)₂, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO₃:BaTiB₂O₆ (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F²)=0.039 for 504 unique reflections. Ba₃Ti₃O₆(BO₃)₂ is isostructural with K₃Ta₃O₆(BO₃)₂. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba₃Ti₃O₆(BO₃)₂ is equal to 95% of that of LiNbO₃.     

Structure of two new borates YCa3(AlO)3(BO3)4 and YCa3(GaO)3(BO3)4

By replacing Mn in YCa₃(MnO)₃(BO₃)₄ with trivalent Al and Ga, two new borates with the compositions of YCa₃(MO)₃(BO₃)₄ (M=Al, Ga) were prepared by solid-state reaction. Structure refinements from X-ray powder diffraction data revealed that both of them are isostructural to gaudefroyite with a hexagonal space group P6₃/m. Cell parameters of a=10.38775(13)Å, c=5.69198(10)Å for the Al-containing compound and a=10.5167(3)Å, c=5.8146(2)Å for the Ga analog were obtained from the refinements. The structure is constituted of AlO₆ or GaO₆ octahedral chains interconnected by BO₃ groups in the ab plane to form a Kagomé-type lattice, leaving trigonal and apatite-like tunnels. It is found that most rare-earth and Cr, Mn ions can be substituted into the Y³⁺ and M³⁺ sites, respectively, and the preference of rare-earth ions to locate in the trigonal tunnel is correlated to the sizes of the M³⁺ ions.     

Thermoanalytical study of the systems PbCO3SrCO3 and PbCO3CaCO3

This study concerns the coprecipitation of the PbCO₃SrCO₃ and PbCO₃CaCO₃ systems in different molar relationships carried out under the same experimental conditions as the PbCO₃BaCO₃ system studied previously. The precipitates obtained were studied by chemical analysis, thermogravimetry, differential thermal analysis and X-ray powder diffraction. It has been established that, for the PbCO₃SrCO₃ system, solid solutions are obtained under all the different experimental conditions and for the PbCO₃CaCO₃ system the precipitates obtained are always mixtures of PbCO₃ and CaCO₃.     

Sm2O3Ga2O3 and Gd2O3Ga2O3 phase diagrams

Four definite compounds exist in the Sm₂O₃Ga₂O₃ binary phase diagram, namely: Sm₃GaO₆, Sm₄Ga₂O₉, SmGaO₃, and Sm₃Ga₅O₁₂. The $\text{3}\text{1}$ compound is orthorhombic (space group Pnna - Z.4) with the cell parameters: a = 11.40₀Å, b = 5.51₅Å, c = 9.07Å and belongs to the oxysel family. Sm₃GaO₆ and SmGaO₃ melt incongruently at 1715 and 1565°C; Sm₄Ga₂O₉ and Sm₃Ga₅O₁₂ have a congruent melting point at 1710 and 1655°C. With regard to the Gd₂O₃Ga₂O₃ system three definite compounds have been identified: Gd₃GaO₆, Gd₄Ga₂O₉, and Gd₃Ga₅O₁₂. Only the garnet melts congruently at 1740°C with the following composition: Gd_3.12Ga_4.88O₁₂. Gd₃GaO₆, and Gd₄Ga₂O₉ melt incongruently at 1760 and 1700°C. GdGaO₃ is only obtained by melt overheating which may yield an equilibrium or a metastable phase diagram.     

RbAuUSe3, CsAuUSe3, RbAuUTe3, and CsAuUTe3: Syntheses and structure; magnetic properties of RbAuUSe3

The compounds RbAuUSe₃, CsAuUSe₃, and RbAuUTe₃ were synthesized at 1073 K from the reactions of U, Au, Q, and A₂Q₃ (A=Rb or Cs; Q=Se or Te). The compound CsAuUTe₃ was synthesized at 1173 K from the reaction of U, Au, Te, and CsCl as a flux. These isostructural compounds crystallize in the KCuZrS₃ structure type in space group Cmcm of the orthorhombic system. The structure consists of layers that contain nearly regular UQ₆ octahedra and distorted AuQ₄ tetrahedra. The infinite layers are separated by bicapped trigonal prismatic A cations. The magnetic behavior of RbAuUSe₃ deviates significantly from Curie–Weiss behavior at low temperatures. For T>200 K, the values of the Curie constant C and the Weiss constant θ_p are 1.82(9) emu K mol⁻¹ and −3.5(2)×10² K, respectively. The effective magnetic moment μ_eff is 3.81(9) μ_B. Formal oxidation states of A/Au/U/Q may be assigned as +1/+1/+4/−2, respectively.     

Thermal decomposition of organo-bielemental vanadium compounds Cp2V(ER3) (ER3 - GeEt3, SnEt3, CH2SiMe3 SeGeEt3)

The thermal decompositon of a number of organo-bielemental vanadium compounds with the general formula Cp₂V(ER₃) (ER₃ - GeEt₃, SnEt₃, CH₂SiMe₃, SeGeEt₃) has been investigated in solids and in solution. The main decomposition products of Cp₂V(SnEt₃) are vanadocene and hexaethyldistannane. Et₃GeH, Et₃GeCp, Cp₂V and CpV(C₅H₄GeEt₃) are formed from Cp₂V (GeET₃) decomposition. Isolated CpV(C₅H₄GeEt₃) is characterized by IR and mass spectra. The decomposition of Cp₂V(CH₂SiMe₃) is accompanied by Me₄Si, Cp₂V and CpV-(C₅H₄CH₂SiMe₃) formation, the latter is identified from the mass spectrum. Triethylgermane, vanadocene, and a diselenide of vanadium are isolated on decomposition of Cp₂V(SeGeEt₃). Based upon the experimental data, mechanisms for the decompositon are proposed.     

Syntheses, structures, and properties of Ag4(Mo2O5)(SeO4)2(SeO3) and Ag2(MoO3)3SeO3

Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) has been synthesized by reacting AgNO₃, MoO₃, and selenic acid under mild hydrothermal conditions. The structure of this compound consists of cis-MoO₂²⁺ molybdenyl units that are bridged to neighboring molybdenyl moieties by selenate anions and by a bridging oxo anion. These dimeric units are joined by selenite anions to yield zigzag one-dimensional chains that extended down the c-axis. Individual chains are polar with the C₂ distortion of the Mo(VI) octahedra aligning on one side of each chain. However, the overall structure is centrosymmetric because neighboring chains have opposite alignment of the C₂ distortion. Upon heating Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) looses SeO₂ in two distinct steps to yield Ag₂MoO₄. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): orthorhombic, space group Pbcm, a=5.6557(3), b=15.8904(7), c=15.7938(7) Å, V=1419.41(12), Z=4, R(F)=2.72% for 121 parameters with 1829 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ was synthesized by reacting AgNO₃ with MoO₃, SeO₂, and HF under hydrothermal conditions. The structure of Ag₂(MoO₃)₃SeO₃ consists of three crystallographically unique Mo(VI) centers that are in 2+2+2 coordination environments with two long, two intermediate, and two short bonds. These MoO₆ units are connected to form a molybdenyl ribbon that extends along the c-axis. These ribbons are further connected together through tridentate selenite anions to form two-dimensional layers in the [bc] plane. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): monoclinic, space group P2₁/n, a=7.7034(5), b=11.1485(8), c=12.7500(9) Å, β=105.018(1) V=1002.7(2), Z=4, R(F)=3.45% for 164 parameters with 2454 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ decomposes to Ag₂Mo₃O₁₀ on heating above 550 °C.     

High-pressure syntheses of TaS3, NbS3, TaSe3, and NbSe3 with NbSe3-type crystal structure

Transition metal trichalcogenides TaSe₃, TaS₃, NbSe₃ and NbS₃ were prepared under the reaction conditions of 2 GPa, 700°C, 30 min. NbSe₃ is exactly the same as that obtained in the usual sealed-tube method. The other products are modifications of each usual phase. They have crystal structures very similar to that of NbSe₃. The lattice parameters are a = 10.02Å, b = 3.48 Å, c = 15.56 Å, β = 109.6° for TaSe₃, a = 9.52 Å, b = 3.35 Å, c = 14.92 Å, β = 110.0° for TaS₃, and a = 9.68 Å, b = 3.37 Å, c = 14.83 Å, β = 109.9° for NbS₃. In spite of the similarity in their crystal structures, these high-pressure phases show a variety of electrical transport properties. TaSe₃ is a superconductor having T_c at 1.9 K. TaS₃ is a semiconductor with two transitions at 200 and 250 K. NbS₃ is a semiconductor with E_a = 180 MeV.     

Intramolecular Hindrances to CCl3 Reorientations in CCl3PCl4 and (CCl3)2PCl3 Crystals

The trigonal bipyramidal structure of trichloromethyl-tetrachlorophosphorane CCl₃PCl₄ and bis(trichloromethyl)trichlorophosphorane (CCl₃)₂PCl₃ molecules with apical CCl₃ groups is responsible for steric hindrances to reorientations of these groups around the C–P bond. The intramolecular barriers to CCl₃ reorientations calculated for the two phosphoranes (Hartree–Fock method using the 6-31G(d) basis set) are 105.9 kJ/mole and 106.6 kJ/mole, respectively. These internal barriers are high enough to block the reorientational motion of the CCl₃ groups, as found previously by ³⁵Cl NQR for the stated crystals.