Pd_2X_2（dpm）_2（X＝NCO~－，CH_3CO_2~－，SCN~－，

采用ＮＭＲ方法考察了室温和低温（－７８～－６０℃）下Ｐｄ２Ｘ２（ｄｐｍ）２（Ｘ＝ＮＣＯ－，ＣＨ３ＣＯ，ＳＣＮ－和ＮＯ，ｄｐｍ＝Ｐｈ２ＰＣＨ２ＰＰｈ２）与Ｈ２Ｓ在ＣＤ２Ｃｌ２或ＣＤＣｌ３中的反应。结果表明，在Ｘ＝ＮＣＯ－和ＣＨ３ＣＯ的情况下，Ｈ２Ｓ优先与这些Ｐｄ配合物的阴离子作用生成相应的共轭酸ＨＸ和Ｐｄ２（ＳＨ）２（ｄｐｍ）２，后者在Ｈ２Ｓ存在下又进一步转化为Ｐｄ２（ＳＨ）２（ｄｐｍ）２（μ－Ｓ）；当Ｘ＝ＳＣＮ－和ＮＯ时，反应则生成结构可能为［Ｐｄ２（Ｈ）（ＳＨ）（μ－ＳＨ）（ｄｐｍ）２］＋的双核Ｐｄ配合物。     

甲烷部分氧化制合成气的钙钛矿型致密透氧膜反应器的数值模拟(英文)

采用等温理论模型,以甲烷催化氧化制合成气为模型反应,模拟非担载钙钛矿型致密透氧膜反应器的性能。分别研究了Ｌａ_０．２Ｂａ_０．８Ｆｅ_０．８Ｃｏ_０．２Ｏ_(３－δ)、Ｌ３０．２Ｓｒ０．８Ｆｅ０．８Ｃｏ０．２Ｏ３－δ和ＳｒＦｅＣｏ０．５Ｏｘ三种透氧速率不同的膜材料、膜反应器的尺寸以及反应工艺条件对ＣＨ４转化率、ＣＯ选择性和Ｈ２／ＣＯ摩尔比的影响,对膜反应实验具有指导意义。     

含硅二硫代磷酸酯的合成及生物活性

硅基甲硫醇Ｒ＾１Ｒ＾２ＣＨ３ＳｉＣＨ２ＳＨ与Ｏ，Ｏ－二烷基二硫代磷酸酯（ＲＯ）２Ｐ（Ｓ）ＳＨ及甲醛可顺利地发生类Ｍａｎｎｉｃｈ缩合反应，利用此反应和硅基甲硫醇与Ｏ，Ｏ－二乙基－Ｓ（２－溴乙基）二硫代磷酸酯的取代反应合成了３７种新的含硅二硫代到酯化合物（ＲＯ）２Ｐ（Ｓ）Ｓ（ＣＨ２）ｎＳＣＨ２ＳｉＣＨ３Ｒ＾１Ｒ＾２（ｎ＝１，２），在初筛浓度下，该类化合物具有一定的杀虫，杀螨活性。     

Pd2X2（dpm）2（X=NCO^—,CH3CO2^—,SCN^—,NO^—3;dpm=Ph2PCH2PPh2）配合…

采用ＮＭＲ方法考察了室温和低温（－７８～－６０℃）下Ｐｄ２Ｘ２（ｄｐｍ）２（Ｘ＝ＮＣＯ＾－，ＣＨ３ＣＯ＾－２，ＳＣＮ＾－和ＮＯ＾－３，ｄｐｍ＝Ｐｈ２ＰＣＨ２ＰＰｈ２）与Ｈ２Ｓ在ＣＤ２Ｃｌ２或ＣＤＣｌ３中的反应。结果表明，在Ｘ＝ＮＣＯ＾－和ＣＨ３ＣＯ＾－２的情况下，Ｈ２Ｓ优先与这些Ｐｄ配合物的阴离子作用生成相应的共轭酸ＨＸ和Ｐｄ２（ＳＨ）２（ｄｐｍ）２，后者在Ｈ２Ｓ存在下又进一步转化为Ｐｄ２（ＳＨ）     

Pd2X2（dpm）2（X=Cl^—,Br^—,I^—）与H2S反应的低温NMR研究

采用低温ＮＭＲ技术考察了配合物Ｐｄ２Ｘ２（ｄｐｍ）２（ｘ＝Ｃｌ＾－，Ｂｒ＾－，Ｉ＾－；ｄｐｍ＝Ｐｈ２ＰＣＨ２ＰＰｈ２）与Ｈ２Ｓ在ＣＤ２Ｃｌ２溶液中的反应，对反应中间体进行了详细的表征。结果表明，反应首先由Ｈ２Ｓ对Ｐｄ２Ｘ２（ｄｐｍ）２的Ｐｄ－Ｐｄ键氧化加成，形成相应的带有Ｐｄ－Ｈ和Ｐｄ－ＳＨ的中间体，该中间体随后脱去Ｈ２并转化为相应的Ｓ＾２－桥联的配合物Ｐｄ２Ｘ２（ｄｐｍ）２（μ－Ｓ）。     

N235二甲苯-醋酸铵-液膜体系萃取Cd(Ⅱ)的研究

本文研究了反萃剂,料液ＨＣｌ浓度、温度、Ｎ２３５浓度对Ｎ２３５－二甲苯－醋酸铵大块液膜体系迁移Ｃｄ＾２＋的影响,当膜相添加不同浓度的表面活性剂Ｓｐａｎ－８０时,测定了膜－料液界面的萃取反应表观速率常数ｋ１和膜－反萃相界面的反萃取表观速率常数ｋ２,并进行了相应的动力学分析。实验证明,Ｃｄ＾２＋的迁称可用两个连续单不可逆的一级反应来描述,在本文的液膜体系中,Ｃｄ＾２＋的跨膜迁移和Ｈ＾＋的同向迁移耦合。     

SO2-4/Z4O2-TiO2-SiO2固体酸催化苯乙烯选择氧化反应的研究

制备了一种ＳＯ＾２－４促进的金属氧化物固体酸ＳＯ＾２－４／ＺｒＯ２－ＴｉＯ２－ＳｉＯ２,并将其用于催化Ｃ６Ｈ５Ｃ２Ｈ３的选择氧化反应,发现该新型固体酸具有较高的活性和选择性,Ｃ６Ｈ５Ｃ２Ｈ３转化率达１０．７３％,Ｃ６Ｈ５Ｃ２Ｈ５Ｏ选择性达２０．７３％。用ＩＲ,ＸＲＤ等方法进行的表征表明,反应的选择氧化活性位可能含有Ｚｒ,Ｓｉ,Ｏ,Ｔｉ等成分。     

聚环氧乙烷（PEO）／壳聚糖（CS）共混膜的醇—水渗透蒸发性能研究

研究了ＥｔＯＨ－Ｈ２Ｏ，ｎ－ＰｒＯＨ－Ｈ２Ｏ，ｉ－ＰｒＯｈ－Ｈ２Ｏ体系在ＣＳ膜和ＰＥＯ／ＣＳ共混膜中的渗透蒸发性能。讨论了料液温度、料液浓度、共混膜组成对分离性能的影响，结果发现ＰＥＯ的掺入能大大提高ＣＳ膜的渗透通量，而分离因子下降。同时从膜材料的聚集态结构出发对相关的渗透蒸发行为进行了讨论。对于ＰＥＯ／ＣＳ共混膜，膜内自由体积的大小是影响分离性能的主要因素，小分子在膜中的渗透蒸发行全为主要是由扩     

聚环氧乙烷（PEO）／壳聚糖（CS）共混膜的醇－水渗透蒸发性能研究

研究了ＥｔＯＨ－Ｈ２Ｏ，ｎ－ＰｒＯＨ－Ｈ２Ｏ，ｉ－ＰｒＯＨ－Ｈ２Ｏ体系在ＣＳ膜和ＰＥＯ／ＣＳ共混膜中的渗透蒸发性能。讨论了料液温度、料液浓度、共混膜组成对分离性能的影响，结果发现ＰＥＯ的掺入能大大提高ｃｓ膜的渗透通量；而分离因子下降。同时从膜材料的聚集态结构出发对相关的渗透蒸发行为进行了讨论。对于ＰＥＯ／ＣＳ共混膜，膜内自由体积的大小是影响分离性能的主要因素，小分子在膜中的渗透蒸发行为主要是由扩散过程控制的。本文还研究了ＰＥＯ的掺入对壳聚塘膜强度的影响以及利用ＤＳＣ谱研究ＰＥＯ掺入后壳聚糖膜聚集态结构的变化。     

Fe—Silicalite—2催化剂表面CO2加氢反应性能的研究

研究了Ｆｅ／Ｓｉｌｉｃａｌｉｔｅ－２催化剂ＣＯ２加氢低碳烯烃反应性能，利用ＣＯ２－ＴＰＤ，ＣＯ２／Ｈ２－ＴＰＳＲ和ＣＯ／Ｈ２－ＴＰＳＲ表征手段，考察了铁含量及ＭｎＯ助剂对Ｆｅ／Ｓｉｌｉｃａｌｉｔｅ－２催化剂ＣＯ２吸附脱附及加氢反应性能的影响，表明随铁含量增加可提高催化剂对ＣＯ２的吸附能力，有利于提高ＣＯ２加氢反应的转化率。     

CdS thin film: Synthesis and characterization

CdS thin films have been deposited by dip technique using succinic acid as a complexing agent. The structural characterizations of films have been studied by X-ray diffraction. X-ray diffraction pattern prove crystallinity of the deposited films that crystallize in the cubic phase of CdS. The films show high absorption and band gap value which were found to be 2.58 eV. The specific conductivity of the film was found to be in the order of 10^?7 (Ω cm)^?1.     

一种在室温合成具有宽带隙CdS的简单方法

采用简单的磁控溅射方法, 在室温合成了CdS多晶薄膜. 在溅射CdS多晶薄膜过程中, 分别在Ar 气中通入0%、0.88%、1.78%、2.58%和3.40% (体积分数, φ)的O₂, 得到不同O含量的CdS多晶薄膜. 通过X射线衍射仪、拉曼光谱仪、扫描电子显微镜、X射线光电子能谱仪、紫外-可见光谱仪对得到的CdS多晶薄膜进行表征.分析结果表明: O的掺入能得到结合更加致密, 晶粒尺寸更小的CdS多晶薄膜; 与溅射气体中没有O₂时制备的CdS多晶薄膜的光学带隙(2.48 eV)相比, 当溅射气体中O₂的含量为0.88%和1.78% (φ)时, 制备得到的CdS多晶薄膜具有更大的光学带隙, 分别为2.60和2.65 eV; 而当溅射气体中O₂的含量为2.58%和3.40% (φ)时, 得到的CdS光学带隙分别为2.50 和2.49 eV, 与没有掺杂O的CdS的光学带隙(2.48 eV)相当; 当溅射气体中O₂的含量为0.88% (φ)时, 制备的CdS多晶薄膜具有最好的结晶质量. 通过磁控溅射方法, 在溅射气体中O₂含量为0.88% (φ)条件下制备的CdS多晶薄膜表面沉积了CdTe 多晶薄膜并在CdCl₂气氛中进行了高温退火处理, 对退火前后的CdTe多晶薄膜进行了表征. 表征结果显示: CdS中掺入O能得到结合更紧密、退火后晶粒尺寸更大的CdTe多晶薄膜. 通过磁控溅射方法, 在CdS制备过程中于Ar 中掺入O₂, 在室温就能得到具有更大光学带隙的CdS多晶薄膜, 该方法是一种简单和有效的方法, 非常适用于大规模工业化生产.     

Pulsed Laser Deposition ZnS Buffer Layers for CIGS Solar Cells

Polycrystalline ZnS films were prepared by pulsed laser deposition （PLD） on quartz glass substrates under different growth conditions at different substrate temperatures of 20, 200, 400, and 600 ℃, which is a suitable alternative to chemical bath deposited （CBD） CdS as a buffer layer in Cu（In,Ga）Se2 （CIGS） solar cells. X-ray diffraction studies indicate the films are polycrystalline with zinc-blende structure and they exhibit preferential orientation along the cubic phase β-ZnS （111） direction, which conflicts with the conclusion of wurtzite structure by Murali that the ZnS films deposited by pulse plating technique was polycrystalline with wurtzite structure. The Raman spectra of grown films show Al mode at approximately 350 cm^-1, generally observed in the cubic phase β-ZnS compounds. The planar and the cross-sectional morphology were observed by scanning electron microscopic. The dense, smooth, uniform grains are formed on the quartz glass substrates through PLD technique. The grain size of ZnS deposited by PLD is much smaller than that of CdS by conventional CBD method, which is analyzed as the main reason of detrimental cell performance. The composition of the ZnS films was also measured by X-ray fluorescence. The typical ZnS films obtained in this work are near stoichiometric and only a small amount of S-rich. The energy band gaps at different temperatures were obtained by absorption spectroscopy measurement, which increases from 3.2 eV to 3.7 eV with the increasing of the deposition temperature. ZnS has a wider energy band gap than CdS （2.4 eV）, which can enhance the blue response of the photovoltaic cells. These results show the high-quality of these substitute buffer layer materials are prepared through an all-dry technology, which can be used in the manufacture of CIGS thin film solar cells.     

Characterization of CdS nanoparticles formed and aggregated in stearic acid Langmuir–Blodgett films by atomic force microscopy

Alternate films, which are composed of stearic acid and CdS nanoparticles were synthesized by exposing Langmuir–Blodgett (LB) films of cadmium stearate (CdSt₂) to H₂S gas at a pressure of 1 Torr. The changes of surface morphology of film with the increased reaction time were directly observed by atomic force microscopy for the first time. Before being exposed to H₂S, the surface of CdSt₂ LB film was homogeneous from microscale down to nanoscale, and it was observed that CdSt₂ molecules formed a well orderly rectangular herringbone lattice structure on the molecular scale. However, after being exposed to H₂S the ordered CdSt₂ molecules gradually changed into a disordered state, and eventually the LB film surface became rough with the apparent feature of bulk structures on the nanoscale. This change in the morphology can be attributed to the aggregation of buried CdS nanoparticles within LB films, which has been confirmed by a structured UV–visible absorption spectrum where the absorption edge is red-shifted about 0.7 eV with respect to bulk CdS. Finally, the aggregation mechanism of CdS in the LB film was analyzed.     

Cauliflower-like CdS microspheres composed of nanocrystals and their physicochemical properties

Cauliflower-like cadmium sulfide (CdS) microspheres composed of nanocrystals have been successfully synthesized by a hydrothermal method using poly(ethylene glycol) (PEG) as the template coordination agent and characterized by a variety of methods. Our experiments confirmed that the size of the CdS microspheres could be easily modified by controlling the chain length of PEG. Powder X-ray diffraction and Raman spectroscopy measurements revealed the cubic structure of the CdS microspheres; morphological studies performed by HR-SEM and HR-TEM methods showed the cauliflower-like structure of the synthesized CdS microspheres. Each microsphere was identified to be created by the self-assembly of CdS nanocrystals and is attributed to the oriented aggregation of the CdS nanocrystals around a polymer-Cd(2+) complex spherical framework structure. X-ray photoelectron spectroscopy (XPS) and energy-dispersive X-ray (EDX) analysis confirmed the stoichiometries of the CdS microspheres. Diffuse reflectance spectrum (DRS) measurements showed that increasing the PEG chain length increased the band gap value of the CdS microspheres slightly, from 1.99 to 2.06 eV. The cauliflower-like CdS microspheres could be applied to photocatalytic degradation studies.     

Cadmium ions and cadmium sulphide particles in γ-titanium dihydrogen phosphate. Synthesis, thermal behaviour and X-ray characterization

Layered compounds with CdS particles supported on the ion-exchanger, γ-titanium dihydrogen phosphate, were prepared by the stepwise reaction of the ion-exchanger and cadmium solution, followed by reaction with H₂S gas. The CdS content on the ion-exchanger is dependent on the timeframe of the H₂S gas flow. The materials obtained were layered, as shown by the X-ray measurements that exhibit both precursor and CdS diffraction peaks. The thermal treatment of the material obtained gives evidence of its stability (≤ 320°C) before the CdS decomposition, which occurs in a single step.      

A single-source route to CdS nanorods

We report the preparation of CdS nanorods using a thiosemicarbazide complex of cadmium [Cd(NH2CSNHNH2)2Cl2]. The precursor was decomposed in tri-n-octylphosphine oxide (TOPO) at 280 degrees C to give TOPO capped CdS nanoparticles; nano-dimensional rods of the material are clearly visible in transmission electron microscopy (TEM); the particles have been further characterised by X-ray diffraction (XRD) and selected area electron diffraction (SAED) and optical measurements.     

CdS Thin Films Deposited by CBD Method on Glass

CdS thin films were prepared by chemical-bath-deposited method and the effect of tempera-ture and time on the properties of CdS thin films was studied. Independent of the deposited temperature, the growth was mainly controlled by the ion-by-ion growth mechanism at the beginning of the film deposition, then the cluster-by-cluster mechanism came to be domi-nant. The growth rate increased faster with the increasing of temperature until the thickness reached the limitation, then thickness instead become thinner. The scanning electron micro-scope results revealed that the morphology of the CdS film changed from pinholes to rough,inhomogeneous surface with increasing deposition time and deposition temperature. The X-ray diffraction results showed the film structure was a mixture of two phases: hexagonal and cubic, and it was very important to controll deposition time to the film's crystal phase. All films in depth of approximate 100 nm existed above 65% transmittance, the absorption edge became 〝red-shift〞 with temperature rising. At 60 and 70 oC, with 20 min deposited-time, the energy band gap was more than 2.42 eV and decreased with time, while at 80 and 90 oC, the energy band gap was less than 2.42 eV and increased little when the time changed from 10 min to 15 min at 80 oC.     

CdS纳米晶@碳点复合物膜的电致化学发光

采用热解柠檬酸法制备碳点(CDs),并将之与表面无包裹剂的CdS纳米晶(CdS NCs)超声复合制备CdS纳米晶@碳点(CdS NCs@CDs)复合物。研究了复合物膜阴极电致化学发光(ECL),探讨了CDs对CdS纳米晶膜ECL增强的机理。CDs分散性良好、尺寸在1.5~4 nm之间;与粒径约为4 nm的CdS纳米晶按体积比2∶3复合后,在360 nm光激发下复合物具有最强的荧光发射且表现为CDs的荧光。同时,复合物膜产生归属于激发态CdS纳米晶的最强的ECL发射,且ECL发光峰起置电势正移至-1.05 V。复合物膜的ECL发射是pH依赖的,在pH值为6时,复合物膜具有最大的ECL强度,为CdS纳米晶膜ECL强度的19倍。这种ECL增强源于CDs能束缚大量电子产生局域电场从而促进近邻CdS纳米晶激发态的形成与弛豫。     

阳离子镍基MOF自组装CdS/PFC-8催化剂用于可见光光催化选择性苯甲醇氧化耦合产氢（英文）

可见光驱动的光催化制氢与有机氧化合成相结合由于其环境友好性和可持续性而极具吸引力,它可以在温和的条件下同时产生清洁的氢气燃料和高价值化学品,而无需牺牲剂。半导体材料和金属有机骨架(MOFs)材料由于其性能和优势,在光催化领域得到了广泛的应用。在这项工作中,我们通过静电自组装成功合成了一种名为Cd S/PFC-8的新型有效催化剂。其中,PFC-8作为镍基金属有机骨架,Cd S/PFC-8复合材料作为无贵金属催化剂,在可见光下具有优异的光催化制氢和苯甲醇氧化性能。对Cd S/PFC-8复合材料进行了一系列催化表征。X射线衍射(XRD)和扫描电子显微镜(SEM)结果表明了Cd S/PFC-8复合材料的成功合成。X射线光电子能谱(XPS)表明了Cd S纳米棒与PFC-8之间存在一定的界面相互作用。通过紫外-可见漫反射光谱(DRS)、光致发光光谱(PL)和电化学测试对光电性能进行了表征,表明Cd S/PFC-8复合材料的可见光响应和光催化可行性。对不同催化剂的光催化实验结果进行比较,在可见光下,Cd S/PFC-8复合材料将H2的产生与苯甲醇的选择性氧化耦合,表现出显著的H2产率3376μmol...