第一性原理研究HC(NH2)2PbI3钙钛矿(三方相VS六方相)的结构及光电特性

采用第一性原理,研究三方及六方相FAPbI₃（FA=HC（NH₂）₂⁺）钙钛矿的结构及光电特性.结果表明,FAPbI₃钙钛矿由三方到六方的形变能够扭转PbI₃骨架,改变Pb-I键合特性,进而改变其禁带宽度值.两种晶体均属于直接带隙半导体,三方相FAPbI₃的直接带隙点位于布里渊区Z（0,0,0.5）对称点,具有较为理想的约1.50 eV的禁带宽度;六方相FAPbI₃的直接带隙点位于Γ（0,0,0）对称点,具有约2.50 eV的禁带宽度.FA离子不直接参与电子跃迁过程,仅仅充当电荷供体为PbI₃骨架提供超过0.7 e的电荷.相比于六方相晶体,三方相FAPbI₃具有更小的载流子有效质量,吸收光谱发生了显著的红移,并且其吸收特性优于六方相FAPbI₃和四方相MAPbI₃（MA=CH₃NH₃⁺）钙钛矿.六方相FAPbI₃比三方相晶系更稳定,FA和PbI₃骨架之间的结合作用力强于MA和PbI₃骨架之间的作用力.     

4-氟苯乙胺基准二维钙钛矿的合成及其电致发光与激光性能

设计并开发了一种兼具电致发光和光学增益性能的准二维钙钛矿材料。通过向三维钙钛矿CsPbBr₃中引入大体积阳离子4-FPEA⁺(4-氟苯乙胺),利用简易的溶液旋涂法,制备了不同n值量子阱混合分布的准二维钙钛矿薄膜。通过紫外可见吸收光谱和光致发光光谱证明调整4-FPEA⁺的添加量可以对量子阱的分布进行有效调控。结合扫描电子显微镜和原子力显微镜证明4-FPEA⁺的加入可以降低薄膜表面粗糙度。当4-FPEA⁺和CsPbBr₃的物质的量之比为0.6时,薄膜的发光强度最高。将该材料应用在发光二极管(light emitting diodes,LEDs)中,结合冠醚作为添加剂辅助钝化缺陷,实现了外量子效率(EQE)为0.98%的绿光LED器件。在激光性能方面,该材料在室温条件下的最低阈值为17.42μJ·cm^-2,增益系数为35 cm^-1。     

铕(Ⅲ)激活的磷酸镧发光性质研究

LaPO₄:Eu³⁺的发射光谱包含较强的Eu³⁺⁵D_o→⁷F₁跃迁发射和较弱的⁶D₁→⁷F₁跃迁发射。主发射峰583nm,对应于Eu³⁺5D_o→⁷F₁跃迁.通过对Eu³⁺的两种跃迁发射强度及荧光寿命和Eu³⁺浓度关系的测定和理论分析,探讨了发光中心Eu³⁺离子同的交叉弛豫和能量迁移机理。     

原位烷基化调控无机-有机杂化类钙钛矿材料的结构及其性能※

无机-有机杂化类钙钛矿材料由于结构可调和独特的光电特性而引起了人们的广泛关注. 通过选用不同的烷基化溶剂, 一步水热法原位合成了两种新型的无机-有机杂化材料——二维(2D)结构的[(Me₃)ODA(Me₃)]₃Pb₅I₁₆ (1)和一维(1D)结构的[H(Et₂)ODA(Et₂)H]Pb₂I₆•H₂O (2) (ODA=4,4-二氨基二苯醚). 化合物1由2D的无机类钙钛矿层[Pb₅I₁₆]^6–和有机阳离子[(Me₃)ODA(Me₃)]²⁺组成, 化合物2由1D无机类钙钛矿链[Pb₂I₆]^2–、有机阳离子[(Et₂)ODA(Et₂)]²⁺和水分子组成. 实验表明, 两种不同维度的化合物虽然都具有典型的半导体性能, 但却表现出不同的化学稳定性以及光、电等物理特性. 其中, 化合物1对波长为400~700 nm的光呈现出明显的光电响应, 而化合物2在对水和有机溶剂表现出良好稳定性的同时, 还表现出优异的湿敏响应性能.     

ALD-Al2O3涂层保护的高抗湿5-氨基戊酸铰链甲胺铅溴钙钛矿薄膜

近年来,混合铅卤钙钛矿材料在光电领域引发的研究热潮引人注目。然而,钙钛矿材料对水和氧气的敏感性严重的阻碍了其实用化进程。在众多的稳定钙钛矿的方法中,利用简单的原子层沉积方法(Atomic layer deposition,ALD)在钙钛矿表面沉积一层保护层的技术具有极大的潜力。而ALD应用的困难在于,在常规的ALD过程中,做为氧源的H2O和O3对铅卤钙钛矿有着腐蚀作用。在本文,我们提出将双官能团的5-氨基戊酸(5-Aminovaleric acid,AVA)引入到CH₃NH₃PbBr₃(MAPbBr₃)钙钛矿晶格层中,形成稳定的铰链结构的2D/3D钙钛矿AVA(MAPbBr₃)2。AVA的引入可以钝化并防止ALD过程中水对钙钛矿的侵蚀,从而成功地直接在钙钛矿表面沉积了Al₂O₃保护层。覆盖了保护层的AVA(MAPbBr₃)2钙钛矿薄膜获得了优异的热稳定性和抗水性。     

基于甲胺客体调制的混价态甲酸铁框架的构筑与磁电行为研究

N-型亚铁磁体可以在场冷时呈现负磁化行为，但在1 T强场场冷时依然能够保持负磁化行为的化合物却很罕见.本工作以CH₃NH₃⁺为客体阳离子，成功构筑了一例红砷镍矿（4⁹.6⁶）（4¹².6³）结构的混价态甲酸铁化合物[CH₃NH₃]_n[Fe^IIIFe^II（HCO₂）₆]_n（1），在1 T强场下呈现负磁化行为.1中甲酸根采用反，反模式连接Fe^II和Fe^III形成三维阴离子框架，八面体配位构型的Fe^II和Fe^III分别处于（4⁹.6⁶）和（4¹².6³）节点，而CH₃NH₃⁺则填充在框架空隙中平衡电荷.量热、介电和单晶X-射线衍射测试结果表明，1中存在由CH₃NH₃⁺无序-有序转变诱导的结构相变并伴随介电弛豫.磁性研究表明Fe^II和Fe^III之间存在较强的反铁磁耦合，但在冷却过程中Fe^II和Fe^III构成的亚晶格磁有序程度存在较大差异，且具有较小自旋的Fe^II磁矩先于Fe^III磁矩有序且平行于外加磁场，导致温度进一步降低时1呈现出负磁化行为，这表明1是一例罕见的N-型亚铁磁体.此外，1在1 T外加冷却场中依然能保持负磁化行为，表明1中存在较强的磁各向异性.值得注意的是，在100 Oe外场下冷却到17 K后，1呈现出正场调制的磁极翻转行为.进一步研究表明，1的场冷磁滞回线呈现不对称形状，并向冷却场方向发生偏转，其有效矫顽力（H_C^eff=（H⁺-H^-）/2）和交换偏置场（H_EB=（H⁺+H^-）/2）分别为21716 Oe和3322 Oe.总之，本研究表明客体分子尺寸和形状能够有效调控红砷镍矿结构中Fe^II的磁各向异性，从而实现较高的磁极翻转场、矫顽力和交换偏置场.     

具有不同电荷和手性的Co(Ⅲ)配合物跨人红细胞膜的动力学研究

研究了4种不同电荷的Co(Ⅲ)金属配合物跨人红细胞膜的动力学,并测定了它们跨人红细胞膜的一级反应动力学速率常数,发现[Co(C₂O₄)₃]^3-的跨膜速率明显高于[Co(en)₃]³⁺,[Co(en)₂(C₂O₄)]⁺和[Co(en)(C₂O₄)₂]^-,后3种配合物的跨膜速率常数随正电荷的减少略有增加,跨膜机制为简单扩散.[Co(C₂O₄)₃]^3-的跨膜速率受阴离子通道抑制剂DIDS明显抑制,抑制率为51.95%,推测其跨膜机制为部分经阴离子通道协同简单扩散过膜.人红细胞摄入L-[Co(C₂O₄)₃]^3-的速率明显大于D-[Co(C₂O₄)₃]^3-,显示了一定的手性选择性.     

微量热法研究过氧化氢酶反应

利用微量热法和热动力学方程研究了过氢化氢酶反应.该反应遵循Michaelis-Menten动力学,298.15K和pH7.0时,其米氏常数、酶转换数以及摩尔反应焓分别为2.36×10^-2mol/L、1.20×10⁴s^-1和-83.67kJ·mol^-1.过氧化氢酶反应后期对底物是一级反应,其总反应速度常数和一级速度常数分别为k_o=6.31×10⁵L·mol^-1·s^-1和k₁=6.31×10⁵/[E_o]s^-1.该反应服从Ogura机理,其酶-底物三元复合物的分解速度常数为6.00×10³s^-1.     

用13CNMR研究星形聚苯乙烯溶液的分子运动(Ⅰ)

用VarianFT-80ANMR谱仪,对结构规则的星形聚苯乙烯在d₄-邻二氯苯和CDCl₃溶液中的¹³CNMR自旋-晶格弛豫时间、线宽和NOE进行了测定。研究了分子量、浓度、溶剂和分子结构对弛豫的影响,并用相关时间的log-X²分布函数模型解释了实验数据。     

(2-羧基苯氧基)苯-1,2-二羧酸构筑的镧系配合物对苯甲醛和阳离子的荧光传感

采用水热法合成了5个稀土配合物[Sm₂(bdbc)₂(phen)₄](1)和[Ln(bdbc)(phen)(H₂O)][Ln=Eu(2), Gd(3), Tb(4), Dy(5), bdbc=(2-羧基苯氧基)苯-1,2-二羧酸根, phen=1,10-邻菲啰啉]. 配合物1是双核分子, 通过氢键和C—H…π作用进一步构筑成一维超分子结构; 配合物2~5是同构的一维双螺旋结构, 通过氢键和C—H…π作用进一步构筑成三维超分子结构. 配合物1, 2, 4和5呈现了Sm³⁺, Eu³⁺, Tb³⁺和Dy³⁺离子的特征发射, 分别对应于Sm³⁺离子的⁴G_5/2→⁶H_J/2(J=5, 7, 9)、 Eu³⁺离子的⁵D₀→⁷F_J(J=1—4)、 Tb³⁺离子的⁵D₄→⁷F_J(J=6, 5, 4, 3)和Dy³⁺离子的⁴F_5/2→⁶H_J/2(J=15, 13)跃迁. 对配合物4的荧光性质进行了表征, 结果表明, 配合物4可用作荧光探针以检测阳离子和苯甲醛.     

Molecular motion in solid ethyltrimethylammonium halides

Proton magnetic resonance spectra have been studied over a wide temperature range for polycrystalline ethyltrimethylammonium halides [C₂H₃N(CH₃)₃]⁺X⁻, where X⁻ = Cl⁻, Br⁻ and I⁻. For the bromide and its ethyl-deuterated analogue, the proton relaxation times T₁ were also measured vs. temperature. Analysis of the experimental data yields information on the activation parameters for molecular motion within the cation and of the cation as a whole. The potential barriers determined increase as anion size decreases.     

Effect of Zn2+ Ions on Upconversion Emission of Er3+ in Zn/Er:LiNbO3 Crystal

The effect of Zn2+ ions codoped on the upconversion emission of Er3+ ions in Er:LiNbO3 crystal under different excitation wavelength was reported.The upconversion emission spectra of Zn/Er:LiNbO3 follo...     

Structures and energetics of C3H6S isomers: a Gaussian-3 ab initio study

Twenty-two isomers/conformers of C₃H₆S^+√ radical cations have been identified and their heats of formation (ΔH_f) at 0 and 298 K have been calculated using the Gaussian-3 (G3) method. Seven of these isomers are known and their ΔH_f data are available in the literature for comparison. The least energy isomer is found to be the thioacetone radical cation (4⁺) with C_2v symmetry. In contrast, the least energy C₃H₆O^+√ isomer is the 1-propen-2-ol radical cation. The G3 ΔH_f298 of 4⁺ is calculated to be 859.4 kJ mol⁻¹, ca. 38 kJ mol⁻¹ higher than the literature value, ≤821 kJ mol⁻¹. For allyl mercaptan radical cation (7⁺), the G3 ΔH_f298 is calculated to be 927.8 kJ mol⁻¹, also not in good agreement with the experimental estimate, 956 kJ mol⁻¹. Upon examining the experimental data and carrying out further calculations, it is shown that the G3 ΔH_f298 values for 4⁺ and 7⁺ should be more reliable than the compiled values. For the five remaining cations with available experimental thermal data, the agreement between the experimental and G3 results ranges from fair to excellent.

Cation CH₃CHSCH₂^+√ (10⁺) has the least energy among the eleven distonic radical cations identified. Their ΔH_f298 values range from 918 to 1151 kJ mol⁻¹. Nevertheless, only one of them, CH₂=SCH₂CH₂^+√ (12⁺), has been observed. Its G3 ΔH_f298 value is 980.9 kJ mol⁻¹, in fair agreement with the experimental result, 990 kJ mol⁻¹.

A couple of reactions involving C₃H₆S^+√ isomers CH₂=SCH₂CH₂^+√ (12⁺) and trimethylene sulfide radical cation (13⁺) have also been studied with the G3 method and the results are consistent with experimental findings.     

Chemical vapor deposition growth of phase-selective inorganic lead halide perovskite films for sensitive photodetectors

Inorganic lead halide perovskites are attractive optoelectronic materials owing to their relative stability compared to organic cation alternatives.The chemical vapor deposition(CVD) method offers potential for high quality perovskite film growth.The deposition temperature is a critical parameter determining the film quality owing to the melting difference between the precursors.Here,perovskite films were deposited by the CVD method at various temperatures between 500-800℃.The perovskite phase converts from CsPb₂Br₅ to CsPbBr₃ gradually as the deposition temperature is increased.The grain size of the perovskite films also increases with temperature.The phase transition mechanism was clarified.The photoexcited state dynamics were investigated by spatially and temporally resolved fluorescence measurements.The perovskite film deposited under 750℃ condition is of the CsPbBr₃ phase,showing low trap-state density and large crystalline grain size.A photodetector based on perovskite films shows high photocurrent and an on/off ratio of ~2.5×10⁴.     

甲胺基-甲脒基混合钙钛矿的第一性原理研究

有机铅卤钙钛矿APbX_3的稳定性是制约其应用的重要因素,对APbX_3钙钛矿中A和X采用不同种类离子混合的化学组分调控是改进其稳定性最有效的方式之一。其中,A位点采用不同比例的甲脒离子(FA)和甲胺离子(MA)是当前研究的热点方向。本文通过第一性原理计算,系统研究了FA_(1-x)MA_xPbI_3体系的结构和光电性质。研究发现FA与MA的混合增加体系的稳定性,其中FA_(0.5)MA_(0.5)PbI_3最稳定。通过分析不同混合比例的结构,揭示了晶格常数随x的增加线性减小;以及带隙随x减小而线性增加。此外,计算结果发现MA所占比例增加时吸收光谱蓝移。研究表明通过FA和MA离子的混合能有效调控钙钛矿的光电性质,从而获得更有效的钙钛矿太阳能电池。     

Interaction of heterocyclic thioamides with tellurium(II) and tellurium(IV). Syntheses and crystal structures of bis[2-(2-thioxo-1,3- thiazolidin-3-yl)-4,5-dihydro-1,3- thiazolium]hexabromotellurate(IV) and tris(1- methylimidazole-2-(3H)-thione)tellurium(II) bromide

Reaction of 1,3-thiazolidine-2-thione with tellurium(IV) in hydrobromic acid medium gave the hexabromotellurate, [C₆H₉N₂S₃]₂²⁺[Te^IVBr₆]²⁻ (3). Reaction of 1-methylimidazoline-2-(3H)-thione (L″) with tellurium(IV), in hydrobromic acid medium, gave the mixed-ligand tellurium(II) complex [Te^IIL″₃Br]⁺Br⁻ (4). The structures of [C₆H₉N₂S₃]₂²⁺[Te^IVBr₆]²⁻ (3) and [Te^IIL″₃Br]⁺Br⁻ were determined by single crystal X-ray diffraction methods. In 3 the unit cell contains [TeBr₆]²⁻ anions and two [C₆H₉N₂S₃]⁺ cations. There is no direct bonding between the metal atom and the cations. In the anion only slight angular deviations from the perfect octahedral geometry are observed. The lone pair of electrons on tellurium(IV) is found to be stereochemically inert. In the cation the two five-membered heterocyclic rings adopt different conformations. In complex 4, in the solid state, the planar [Te^IIL″₃Br]⁺ cation and Br⁻ anion are held together by ionic interactions. In the cation, L″ is bonded to the central tellurium atom through the sulphur atom.     

Reactivity of tri- and tetra-nuclear ethylidyne cyclopentadienylcobalt clusters towards protonic acids

The bis(μ₃-ethylidyne) tricobalt cluster [(CpCo)₃(μ₃-CCH₃)₂] (1b) is protonated by trifluoroacetic acid to give the dicobalt edge-protonated cation [H(CpCo)₃(μ₃-CCH₃)₂]⁺ [lb + H]⁺. Protonation of the μ₃-ethylidyne tetracobalt cluster hydride [H(CpCo)₄(μ₃-CCH₃)] (3) takes place in two consecutive steps. At low temperature [H₂(CpCo)₄(μ₃-CCH₃)]⁺ [3 + H]⁺ is formed first, and is then slowly converted into [H₃(CpCo)₄(μ₃-CCH₃)]²⁺ [3 + 2H]²⁺ by an excess of acid. As judged by the ¹H NMR data and the crystal structure of [3 + X]⁺[(CF₃COO)₂X]⁻ (X = H or D) the endo hydrogens in [3 + H]⁺ and [3 + 2H]²⁺ occupy μ₃-(Co₃) face capping hydridic positions. The cations [1b + H]⁺ and [3 + H]⁺ show hydride fluxionality in solution, which in the case of [3 + H]⁺ can be frozen out on the NMR timescale at low temperature (ΔG ^≠ (203 K) = 40.8 kJ/mol). The structure of [3 + X]⁺ [(CF₃COO)₂X]⁻ (X = H or D) was determined by X-ray crystallography. One of the hydrides/deuterides is located on the crystallographic mirror plane, capping a tricobalt face of the cluster cation. The other endo hydrogen atom is believed to be disordered between the other two μ₃-(Co₃) sites, which are related by space group symmetry. Deuteronation of 3 shows a strong normal kinetic deuterium isotope effect. From the temperature independence of the ¹H NMR spectrum of [3 + 2D]²⁺ a non-fluxional solution structure can be inferred. In all the systems studied, hydridic (μ₂- or μ₃-) sites are thermodynamically preferred to possible isomeric agostic CoHC or Co₂HC sites for the endo hydrogens. Agostic interactions cannot, however, be ruled out in transient intermediates during the course of the protonations.     

The discrimination between triplet state and radical cation in the pulse radiolysis of bithiophene in CCl4

The triplet state (³2T) and the radical cation (2T⁺√) of 2,2′-bithiophene (2T) are characterized by pulse radiolysis in CCl₄. Two main absorption bands at 360 and 420 nm are respectively attributed to ³2T* and to 2T⁺√. The triplet, induced in an excited state through a Förster mechanism, undergoes a conformational rearrangement (k₆=(6.8±0.9)×10⁶ s⁻¹). The radical cation is produced both through a resonance charge transfer and a second diffusional process; the two oxidizing species are respectively CCl₄⁺√ and (CCl⁺₃Cl⁻)_solv through the mediation of a singlet excited state, ¹2T*.     

A quantum mechanical analysis on the selective production of the oxygen atom fine-structure states along asymmetric resonances in OH predissociation

Predissociation of the A ²Σ⁺ state is treated by an exact theory employing two frame transformation matrices, each of which connects the atomic term limits (O(³P) and O(¹D)) to the correlating adiabatic Born—Oppenheimer states. Resonances corresponding to the higher (v 7) rovibrational levels of the A ²Σ⁺ state are predicted to have asymmetric (Fano-type) profiles. The branching ratios of O(³P_j, J = 0, 1, 2) are shown to be influenced by nonadiabatic interactions in the Franck—Condon region between the A ²Σ⁺ and dissociative ⁴Σ⁻, ²Σ⁻ and ⁴Π states. The branching ratios show a strong variation along asymmetric resonances, while remaining energy independent along Lorentzian resonances.