单步电沉积法制备CuInS2薄膜

采用单步电沉积法在Mo基底上制备了高质量的CuInS2薄膜. 用X射线衍射仪(XRD)和扫描电子显微镜(SEM)表征了样品的结构和形貌, 研究了沉积电位、退火温度、pH值、反应物浓度等工艺条件对制备的CuInS2薄膜形貌、组分及性能的影响. 制备的CuInS2薄膜致密平整, 呈黄铜矿结构, 晶粒大小为1-2 μm. 用紫外-可见光分光光度计测试了其光学性能, 计算得到常温下禁带宽度为1.41 eV, 非常适合用作薄膜太阳电池的吸收层材料.     

Preparation and Characterization of CuInS2 Thin Films for Solar Cells by Chemical Bath Deposition

Recent years, chalcopyrite semiconductors have been successfully applied as absorber layers for polycrystalline thin-film solar cells. Among the ternary compound semiconductors, CuInSz thin films with a direct bandgap of about 1.50eV and a large absorption coefficient in the range of 10^4-10^5cm^-1[1] are one kind of the most promising optical absorbers for high efficiency thin film solar cells.     

Synthesis of CuInS2@CdS Core‐Shell Nanocrystals

CuInS₂@CdS core‐shell nanocrystals were prepared in a wet chemical process. Transmission electron microscope (TEM), x‐ray energy dispersive spectroscopy (EDAX), x‐ray diffraction (XRD), absorption, and photoluminescence (PL) spectra were used to confirm the formation of the CuInS₂@CdS core‐shell structure. The growth of CdS shell not only increased the PL intensity, but also restrained the transformation of CuInS₂ from nanoparticles to nanorods after annealing, which was attributed to an effective chemical passivation of the CuInS₂ core by the CdS shell.     

CuInS2纳米晶的结构、形貌与光学性能研究

采用A-Pot法, 以乙酰丙酮铜[Cu(acac)₂]为铜源, 硬脂酸铟[In(St)₃]为铟源, 正十二硫醇(DDT)为硫源和稳定剂, 1-十八烯(ODE)为溶剂, 在250 ℃条件下, 反应50 min, 合成了CuInS₂粉体. 用X射线粉末衍射仪(XRD)、透射电子显微镜(TEM)、能量分散光谱仪(EDS)、X射线光电子能谱(XPS)等对粉体的结构、形貌、相组成进行表征. 结果表明: 产物为四角晶系的黄铜矿结构, 棒状CuInS₂纳米晶的直径为2 nm, 长约70 nm. 通过Z-Scan技术对分散在正己烷中CuInS₂纳米棒的三阶光学非线性进行测试, 在入射波长为770 nm的条件下, 得出三阶光学非线性折射率γ、三阶光学非线性吸收系数β以及三阶光学非线性极化率χ⁽³⁾分别为1.76×10^－17 m²/W, 7.95×10^－11 m/W和8.60×10^－12 esu.     

耦联剂辅助吸附法制备CuInS2量子点敏化太阳电池

分别以CuI 和InAc3 作为铜源和铟源, 十二硫醇(DDT)作为硫源, 采用直接加热法合成不同尺寸的CuInS₂ (CIS)量子点. 运用X射线衍射(XRD), 拉曼光谱(Raman), 高分辨率透射电镜(HRTEM), 紫外-可见(UVVis)吸收光谱表征其相结构、形貌及光学性能. 结果表明: 制备的CIS量子点为黄铜矿结构, 且随着时间的延长, 量子点逐渐长大, 吸收光谱的激子吸收峰逐渐红移, 表现出量子尺寸效应. 采用巯基乙酸为双功能耦联剂辅助吸附法制备CIS敏化的TiO₂薄膜. 通过衰减全反射红外光谱(ATR-FTIR)分析得出, 巯基乙酸上的羧基与TiO₂表面羟基连接, 另一端上的巯基代替长链的DDT与CIS 耦联, 将CIS 成功锚定在TiO₂表面. 该方法不仅操作简单, 而且容易实现CIS在TiO₂表面的吸附. 太阳电池光电性能测试表明, 粒径大小约为3.6 nm的CIS量子点表现出最优的吸附能力以及光电转换性能. 进一步采用连续离子吸附层法对CIS敏化的TiO₂薄膜进行CdS包覆, 光电转换性能大大提高, 其效率达到2.83%, 这主要源于CdS的包覆钝化了CIS 的表面缺陷, 有效地降低了电子复合.     

溶剂热法合成CuInS2-ZnS固溶体及其光催化分解水制氢性能

采用乙二胺为溶剂,硫粉为硫源,在高压反应釜中于200 ℃合成了纳米尺度的CuInS2-ZnS四元硫化物固溶体. 对产物的晶相转变研究发现, ZnS中引入少量In3+离子即可使ZnS由立方相转变为六方相,而且随着In3+引入量的增加, ZnS的粒径逐渐减小. 在可见光(λ>420 nm)照射下,对不同x值的(CuIn)xZn2(1-x)S2固溶体催化剂的光催化活性考察发现, (CuIn)0.09Zn1.82S2催化剂在含有S2--SO2-3牺牲试剂的水溶液中表现出最高的光催化分解水产氢活性. 循环实验表明,该催化剂反应 20 h 后光催化活性没有明显降低.     

基于S-型光催化机制CuInS2内嵌中空凹面氮化碳光催化分解H2O制H2（英文）

光催化解离H2O合成H2是绿色可再生的太阳能光子能量转换策略之一.目前,增强光催化材料对太阳能光子的捕获并将之有效利用仍然是一个具有挑战性的课题.光催化解离H2O反应包括三个过程:太阳能光子能量促使光生电子在半导体材料带隙中的跃迁;光生电子定向传输;光生电子与吸附在半导体材料表面的H2O分子发生反应.第一过程需要强的太阳光子捕获能力以产生足够的光生载流子;第二、三过程在动力学上反映了光生载流子在各个竞争过程中能否有效利用的问题,如光生电子迁移与H2O作用的速度很慢(~μs),而电子与空穴的复合速度快(~ps).目前研究者很难协调半导体材料的电学和光学特性以满足光生载流子在热力学和动力学两方面的要求.g-C3N4是由C、N原子通过sp2杂化组成的二维π共轭体系.当g-C3N4结构偏离二维平面时,共轭体系的π电子由凹面迁移到凸面,促使凹、凸面形成表观电势差,有利于电子的定向传输.本文通过卷曲sp2杂化离域均三嗪体系偏离二维平面,得到空心凹面g-C3N4结构,便捷地优化了半导体的电子结构.将CuInS2嵌入生长于空心g-C3N4的凹面,所构成的半导体光催化材料CuInS2@C3N4展现了增强的光捕获能力,以及电子定向传输转移能力.结合XPS、光电流测试、电化学阻抗谱、稳态及瞬态荧光等表征手段揭示空心g-C3N4凹、凸面表观电势差驱动光生电子以S-型光催化作用机制从CuInS2的Cu 2p向g-C3N4的N 1s的路径转移.因而,所构建的CuInS2@C3N4在可见光激发下产氢效率提高到373μmol·h^?1·g^?1,其产氢效率分别是二维平面g-C3N4负载1 wt%Pt和3 wt%Pd效率的1.57倍和1.35倍,表明空心g-C3N4凹、凸面电势差可以显著地促进光生电子分离和利用率,从而提高光催化解离水制氢效率.本文可增强g-C3N4的可持续太阳能转换性能,也适用于其他半导体材料以替代贵金属光催化体系,降低光催化产氢技术成本,促进光催化技术的应用.     

Structures and Vibrational Spectra of C_2 and LaC_2~ Clusters

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Adsorption properties and photocatalytic activity of TiO2 and La-doped TiO2

Photocatalysts of TiO₂ and La-doped TiO₂ were prepared by calcining the pure TiO₂ sols and the sols mixed with La(NO₃)₃⋅6H₂O at 873 K, respectively. These photocatalysts were characterized by X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), scanning electron microscopy (SEM) and N₂ adsorption-desorption isotherms measurement. As results, the BET surface area, pore diameter, mesopore volume and micropore volume slightly increased, while the crystallite size and the phase structure were little affected by lanthanum doping. The equilibrium adsorption of methylene blue (MB) on the photocatalysts were measured in a dark room. The adsorption isotherms were confirmed to fit to the Langmuir theory. Photocatalytic activities of the photocatalysts were studied by employing the photocatalytic degradation of MB in water and degradation of acetaldehyde in air under UV-irradiation using a black light. Kinetic analysis revealed that the rate controlling steps could be the surface reaction of the adsorbed MB on the catalyst surface for MB degradation and the reaction of adsorbed acetaldehyde with the gaseous acetaldehyde for degradation of acetaldehyde, respectively.     

Synthesis and characterization of diblock copolymer of butadiene and 2-ethyl-2-oxazoline

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Chemical and enzymatic synthesis of 2-(2-carbamoylethyl)- and 2-(2-carboxyethyl)aziridines and their conversion into δ-lactams and γ-lactones

Treatment of 1-arylmethyl-2-(2-cyanoethyl)aziridines with a nitrile hydratase afforded the corresponding 2-(2-carbamoylethyl)aziridines, which underwent rearrangement into 5-hydroxypiperidin-2-ones upon heating under microwave irradiation. In addition, treatment of 2-(2-cyanoethyl)aziridines with a nitrilase selectively afforded 5-hydroxypiperidin-2-ones in good yields. On the other hand, chemical hydrolysis of 2-(2-cyanoethyl)aziridines using KOH in EtOH/H(2)O furnished the corresponding potassium 3-(aziridin-2-yl)propanoates, which, upon acidification with acetic acid, smoothly rearranged into 4-(aminomethyl)butyrolactones.     

Thermal and calorimetric investigations of M(IO3)2·2H2O forM 2+=Ni2+ and Zn2+ and their deuterated analogues

The thermal dehydration and decomposition of M(IO₃)₂·2H₂O (M ²⁺=Ni²⁺ and Zn²⁺) and their deuterates were investigated by DTA and DSC methods. The data obtained confirm their onestage dehydration and their decomposition to the respective oxides. Ni(IO₃)₂·2H₂O and Ni(IO₃)₂·2D₂O, were more stable than Zn(IO₃)₂·2H₂O and Zn(IO₃)₂·2D₂O. A considerable isotope effect was observed in relation toT _deh for Ni(IO₃)₂·2H₂O and Ni(IO₃)₂·2D₂O, which was explained by the presence of structural changes well differentiated from the dehydration process for the deuterate. The data obtained for both pairs of dihydrates were used to determine ΔH _f ^o for Ni(IO₃)₂·2H₂O and Ni(IO₃)₂·2D₂O.     

Isomer- and species-selective infrared spectroscopy of jet-cooled 7H- and 9H-2-aminopurine and 2-aminopurine·H2O clusters

The infrared (IR) spectra of the supersonic-jet cooled 9H- and 7H-tautomers of 2-aminopurine (2AP) and of the 9H-2-aminopurine·H(2)O monohydrate clusters have been measured by mass- and species-selective IR-UV double resonance spectroscopy in the 3200-3900 cm(-1) region, covering the N-H and O-H stretching vibrations. The spectra are complemented by density functional (B3LYP and PW91) and by second-order M?ller-Plesset (MP2) calculations of the electronic energies and vibrational frequenciesof the respective 2AP tautomers and clusters. The 9H- and 7H-2-aminopurine tautomers were definitively identified by the shifts of their NH and NH(2) symmetric and asymmetric stretching frequencies and by comparison to the B3LYP/TZVP calculated IR spectra. The H-bond topologies of the two previously observed 9H-2-aminopurine·H(2)O isomers (Sinha. R. K.; et al. J. Phys. Chem. A2011, 115, 6208) are definitively identified as the "sugar-edge" isomer A and the "trans-amino-bound" isomer B by comparing their IR spectra to the calculated frequencies and IR intensities of the cluster isomers A, B, C, and D, as well as to the IR spectrum of 9H-2AP. The sugar-edge isomer A involves N9-H···OH(2) and HOH···N3 hydrogen bonds and is predicted to be the most stable form. The amino-bound isomer B involves NH(2)···OH(2) and HOH···N1 hydrogen bonds and is calculated to lie 2.5 kJ/mol above isomer A. The H-bond topology of the "cis-amino-bound" isomer C is symmetrically related to isomer B, with a hydrogen bond to the N3 of the pyrimidine group. However, it is calculated to lie 7 kJ/mol above isomer A and indeed is not observed in the supersonic jet. Isomer D involves a single H-bond to the N7 position, is predicted to be 14 kJ/mol above A and is therefore not observed.     

A combined experimental and model analysis on the effect of pH and O2(aq) on γ-radiolytically produced H2 and H2O2

The effects of pH and dissolved O₂ on the γ-radiolysis of water were studied at an absorbed dose rate of 2.5 Gy s⁻¹. Argon- or air-saturated water with no headspace was irradiated and the aqueous samples were analyzed for molecular radiolysis products (H₂ and H₂O₂) as a function of irradiation time. The experimental results were compared with computer simulation results using a comprehensive water-radiolysis kinetic model, consisting of the primary radiolysis production, subsequent reactions and related acid–base equilibria. Both the experimental and computer model results were discussed based on the steady-state kinetic analysis of smaller reaction sets consisting of key production and removal reactions. While the main production path for a water decomposition product is the primary radiolysis, the main removal path varies. For H₂O₂ the main removal path is the reactions with e_aq⁻ and OH, whereas for H₂ it is the reaction with OH. As a result, the presence of a dissolved species, or a change in chemical environment, affects the concentrations of H₂O₂ and H₂ through interaction with radicals e_aq⁻ and OH. Over a wide range of conditions, there exist quantitative but simple relationships between the radical and the molecular product concentrations. The experimental and model analyses show that dissolved oxygen increases the steady-state concentrations of H₂O₂ and H₂ by reacting with OH and e_aq^–, and the impact of oxygen is more noticeable at pH below 8. The steady-state concentrations of water decomposition products are nearly independent of pH in the range 5–8. However, raising pH above the pKa value of the acid–base equilibrium of H (⇆e_aq⁻+H⁺) significantly increases [H₂O₂] and [H₂] at the expenses of [OH] and [e_aq^–]. At pH >10, the radiolytical production of O₂ becomes significant, but at a finite rate. This considerably increases the time for the irradiated system to reach a steady state, and is responsible for different impacts on [H₂O₂] and [H₂] due to radically produced O₂, compared to impacts due to initially dissolved O₂. Model sensitivity analysis has shown that at higher pHs (pH >10) transient species such as O₂⁻ and O₃⁻ play a major role in determining the steady-state concentration of molecular products H₂ and H₂O₂. Further validation of the water radiolysis model, particularly at higher pHs, is also discussed.     

The HRuCCH, RuCCH2, and Ru-η2-C2H2 molecules: infrared spectra and density functional calculations

Laser-ablated ruthenium atoms undergo reaction with acetylene during condensation in excess neon and argon matrices to form a metallacycle complex, insertion into the C-H bond, and rearrangement to the vinylidene complex. The subject molecules were identified by (13)C(2)H(2) and C(2)D(2), isotopic substitutions and density functional theory (DFT) frequency calculations. The HRuCCH molecule is described by Ru-H, CH, and CC stretching modes and CCH deformation modes. A very strong CC double bond stretching, weak CH stretching, and CCH deformation frequencies were observed for the Ru═C═CH(2) complex. The metallacycle Ru-η(2)-(C(2)H(2)) is characterized through CC double bond stretching, CH stretching and CCH deformation modes. The reaction mechanism for formation of the Ru═C═CH(2) complex was investigated by B3LYP internal reaction coordinate calculations, and the hydrido-alkyny complex is the rate-determining step. The delocalized three-center-four-electron π bond using the Ru 4d(xz) electron pair contributes to the C-C π* orbital and provides stabilization energy (ΔE((2)), second-order perturbation) for the vinylidene Ru═C═CH(2) complex.     

Thermal and calorimetric studies of M(IO3)2·6H2O and M(IO3)2·6D2O forM 2+=Ca2+ and Sr2+

Thermal and calorimetric studies were carried out on M(IO₃)₂·6H₂O and M(IO₃)₂·6D₂O forM ²⁺=Ca²⁺ and Sr²⁺, using DTA and DSC methods. The thermal behaviour of the ordinary and deuterated hydrates is outlined and the differences observed between them are discussed. The enthalpies of the phase transitions were determined. The H _f ^o for Ca(IO₃)₂·6H₂O, Ca(IO₃)₂·6H₂O(D₂O) and Sr(IO₃)₂·6H₂O(D₂O) were calculated from the H _deh data and comments are made on the isotope effect observed.

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Zusammenfassung Mittels DTA- und DSC-Methoden wurden Me(IO₃)₂·6H₂O und Me(IO₃)₂·6D₂O (mitMe ²⁺=Ca²⁺ und Sr²⁺) thermisch und kalorimetrisch untersucht. Es wird ein Überblick über das thermische Verhalten ordentlicher und deuterierter Hydrate gegeben, in dem auch die Unterschiede zwischen beiden diskutiert werden. Die Enthalpien der untersuchten Phasenumwandlungen wurden bestimmt. Aus den Daten für H_deh wurde H_f von Ca(IO₃)₂·6H₂O, Ca(IO₃)₂H₂O(D₂O) und Sr(IO₃)₂·6H₂O(D₂O) berechnet und Bemerkungen zum beobachteten Isotopeneffektes gemacht.

     

Semi-Empirical and DFT Studies on Structures and Spectra for C78（CH2）2

Eighteen possible isomers of C78（CH2）2 weTe investigated by the INDO method. It was indicated that the most stable isomer was 42,43,62,63-C78（CH2）2, where the -CH2 groups were added to the 6/6 bonds located at the same hexagon passed by the longest axis of C78 （C2v）, to form cyclopropane structures. Based on the most stable four geometries of C78（CH2）2 optimized at B3LYP/3-21G level, the first absorptions in the electronic spectra calculated with the INDO/CIS method and the IR frequencies of the C-C bonds on the carbon cage computed using the AM1 method were blue-shifted compared with those of C78 （C2v） because of the bigger LUMO-HOMO energy gap and the less conjugated carbon cage after the addition. The chemical shifts of ^13C NMR for the carbon atoms on the added bonds calculated at B3LYP/3-21G level were moved upfield thanks to the conversion from sp^2-C to sp^3-C.     

Reaction of 2-alkoxycarbonylmethyl derivatives of δ2-oxazoline and δ2-imidazoline and their tautomers with 4-nitrobenzonitrile N-oxide

It was established that 2-alkoxycarbonylntethylene derivatives of oxazolidine and imidazolidine react readily with 4-nitrobenzonitrile N-oxide; the reaction takes place at the methylidyne carbon atom to give intermediate oximes, which can then undergo cyclization to isoxazoles. Their tautomers —benzimidazole and ² -oxazoline derivatives —react with considerably greater difficulty; in the first case the reaction takes place at a different center, viz., the ring nitrogen atom.Translated from Khimiya Geterotsiklicheskikh Soedinenii, No. 5, pp. 681–684, May, 1991.     

Vibrational spectroscopic study of the hypophosphite and phosphite anions,H2PO2−2 and HPO2−3, and of their deuteriated analogues in the solid state and in aqueous solution

A full vibrational spectroscopic study of sodium hypophosphite, sodium phosphite and their deuteriated analogues has been made. The vibrations characteristic of the hypophosphite anion have been assigned and the presence of a previously unreported band has been established for the Raman spectrum of the aqueous solution. The first Raman study of deuteriated sodium phosphite has been undertaken and a full vibrational assignment is given.