2-芳胺基-3H-1,3,4-噻二唑-5-硫醇类介离子化合物的X射线光电子能谱研究

用XPS表征2-芳胺基-1,3,4-噻二唑-5-硫酮(1)在ω-溴代-ω-(1H-1,2,4-三唑)-苯乙酮诱导下生成的2-芳胺基-3H-1,3,4-噻二唑-5-硫醇类介离子化合物(4).结果表明,化合物4分子中的C_1s,N_1s,S_2p电子结合能均高于化合物1,尤其以N_1s,S_2p结合能谱最为特征.例如在含3个氮原子的化合物4中由于噻二唑环的两个氮环境不同,故产生3个峰,而在与其结构相近的对照物1中,由于噻二唑环的两个氮环境相近,故产生2个峰.S_2p诸状态结合能加合值化合物4均大于化合物1,在化合物4中均是杂环内硫大于杂环外硫.     

ABO3钙钛矿型复合氧化物光催化活性与B离子d电子结构的关系

在ABO₃钙钛矿型复合氧化物中,B离子的d电子结构对B_3d-O_2p之间的电荷转移能ΔCT及B-O之间的结合能起着关键作用,是影响ABO₃复合氧化物光催化活性的一个重要因素.本文以研磨法和柠檬酸法合成了系列LaBO₃(B=Ti-Co),并结合光催化降解实验和光声光谱图分析得出:LaBO₃光催化活性随B离子3d电子数的递增而逐渐增加.     

弛豫铁电体结构起伏与弛豫性研究

制备了铅基弛豫铁电体0.9Pb(Mg_1/3Nb_2/3)O₃-0.1PbTiO₃和Pb(Zn_1/3Nb_2/3)O₃基陶瓷. 铅基弛豫铁电体PMNT, PZN基陶瓷弛豫过程可用局域冻结模型描述. 在微畴-宏畴转变过程中, 弛豫铁电体产生结构起伏; 在相同的频率条件下, 弛豫铁电体的结构起伏程度越大, 弛豫程度越低. 在微畴-宏畴转变过程中, 随微畴的增大, 弛豫铁电体的弛豫特性减弱或消失.     

NO与NO2在ZnO表面吸附的密度泛函理论研究

采用 DMol ³ 模块中广义梯度密度泛函理论(GGA)的Perdew-Burke-Ernzerh(PBE)方法研究含能材料分解气体产物NO, NO₂在ZnO(10 \bar{1} 0)表面的吸附和NO₂解离生成NO和O的过程. 结果表明, 优化后的吸附构型显示Zn顶位为稳定吸附位点, NO₂的吸附能大于NO. 态密度图分析结合差分电荷密度图表明, NO的N原子与表面Zn有相互作用, 电荷从NO转移到表面; NO₂的N_2p, O_2p轨道与表面Zn_3d轨道发生杂化, NO₂附近积累大量负电荷. 过渡态搜索显示NO₂的解离需跨过较高能垒, 不易进行.     

ZnO-TiO2和WO3-TiO2复合薄膜光催化剂的制备与性能

采用溶胶一凝胶法在多孔钛片上制备了 ZnO-TiO₂和WO₃-TiO₂复合半导体光催化剂,用甲基橙的光催化降解反应对所得薄膜的催化活性进行评价,并通过XRD和DTA等手段对样品进行了表征.结果表明,ZnO和WO₃的掺入降低了TiO₂的相转变温度,ZnO适宜掺杂量为0.1 mol%, WO₃适宜掺杂量为0.5 mol%, ZnO-TiO₂和WO₃-TiO₂复合薄膜比纯TiO₂薄膜光催化活性分別高出77.0%和96.7%.     

异质结型光催化膜的活性及其机理研究

采用浸渍提拉法制得TiO₂,ZnO,Fe₂O₃,ZnO/TiO₂,TiO₂/ZnO,Fe₂O₃/TiO₂和TiO₂/Fe₂O₃石英玻璃基底负载膜.光催化降解亚甲基蓝实验表明,TiO₂和ZnO具有良好的光催化活性,Fe₂O₃活性较差.但形成异质结后,TiO₂和Fe₂O₃的光催化降解能力发生明显的变化.用254nm紫外光光照后,TiO₂,ZnO和Fe₂O₃等3种氧化物膜与水的接触角均有不同程度的降低,TiO₂表现出超亲水性,ZnO/TiO₂和Fe₂O₃/TiO₂膜与水的接触角小于对应的单纯ZnO和Fe₂O₃膜与水的接触角,其中Fe₂O₃/TiO₂表面出现超亲水性.瞬态光电导谱的少数载流子寿命的测定表明,异质结势垒电场能有效地增强光生电子-空穴对的分离效率.根据能带理论建立的两组异质结能带模型可合理地解释实验结果.     

铁酸锌(311)表面结构的密度泛函理论研究

利用原子层沉积技术（ALD）合成了铁酸锌（ZnFe₂O₄）纳米颗粒。基于密度泛函理论和原子热力学的方法,计算了ZnFe₂O₄的结构、磁性和电子性质,研究了ZnFe₂O₄（311）面六种不同终结面的稳定性与氧化学势和锌化学势的关系。结果表明,ZnFe₂O₄是具有正尖晶石结构的半导体,禁带宽度为1.91 eV,且具有反铁磁性。在ZnFe₂O₄可以稳定存在的化学势范围内,O₁、O₂、Fe₂、Zn₂四种终结面可以稳定存在,且具有不同的稳定区间。在富锌条件下（△μ_Zn=0 eV）,O₁终结面在大部分O化学势范围内最稳定,在贫锌条件下（△μ_Zn=-3.88 eV）,O₂终结面变得最稳定。     

前驱体物相转变对浆态床合成甲醇催化剂活性的影响

采用并流共沉淀法, 通过考察老化温度, 研究CuO/ZnO/Al₂O₃催化剂前驱体晶相及组成的变化对浆态床催化合成甲醇的反应活性的影响. 结果表明, 前驱体的物相转变对浆态床合成甲醇活性影响显著, 单斜晶系锌孔雀石(Cu,Zn)₂CO₃(OH)2和斜方晶系绿铜锌矿(Cu,Zn)₅(CO₃)₂(OH)₆晶体是产生高活性催化剂的主要物相. 随着Cu²⁺/Zn²⁺进入Zn₅(CO₃)₂(OH)₆/Cu₂CO₃(OH)₂晶格, 离子同晶取代量增加, 催化剂前驱体中形成了固定铜锌比的锌孔雀石和绿铜锌矿物相. 焙烧后催化剂比表面积增大, CuO-ZnO固溶体协同作用加强, 浆态床催化合成甲醇的活性提高.     

Sb2S3纳米粒子修饰ZnO纳米片微纳分级结构的光电化学性能

采用恒电位方法,选择氯化钾和乙二胺(EDA)为添加剂,在氧化铟锡(ITO)导电玻璃上制备了高度有序的ZnO纳米片阵列,通过二次电沉积得到了ZnO纳米片上生长纳米棒的微纳分级结构.利用化学浴沉积法在ZnO基底上沉积Sb₂S₃纳米粒子制备出了Sb₂S₃/ZnO纳米片壳核结构和Sb₂S₃/ZnO微纳分级壳核结构.利用扫描电子显微镜(SEM)、X射线衍射(XRD)、紫外-可见(UV-Vis)吸收光谱、瞬态光电流等对其形貌、结构组成和光电化学性能进行了表征和分析.结果表明, Sb₂S₃/ZnO纳米片上生长纳米棒分级壳核结构的光电流明显高于Sb₂S₃/ZnO纳米片壳核结构.在Sb₂S₃/ZnO纳米片壳核结构和Sb₂S₃/ZnO微纳分级壳核结构的基础上旋涂一层P3HT薄膜形成P3HT/Sb₂S₃/ZnO复合结构,以上述复合结构薄膜为光活性层组装成杂化太阳电池,其中, P3HT/Sb₂S₃/ZnO分级壳核结构杂化太阳电池的能量转换效率最高,达到了0.81%.     

氧元素的同素异形体*

对氧的同素异形体进行了梳理,简要叙述了“固态O₂和四聚氧(O₄)”的制备、结构与晶型转变。其中固态O₂相变涉及的研究较多,在超高压下,固态O₂从绝缘体变为金属态;在极低温度下,固态O₂又转变为超导体。采用以“相变”为主线对固态O₂的6种晶体学相进行了概述,并简要评述了O₄(四聚氧)的结构与性质。     

Ab initio calculations for the Zn 2s and 2p core level binding energies in Zn oxo compounds and ZnO

The Zn 2s and 2p core level binding energies of ZnO and a few Zn oxo compounds containing Zn in its oxidation state +2 were calculated by means of wave function based quantum chemical ab initio methods. The computations were performed at two levels of approximation. First, Hartree-Fock calculations were carried out for the ground state of the neutral systems yielding the "initial state" effects, i.e. the shifts of the core level binding energies due to the changes in the chemical environment of the Zn atom under consideration (Koopmans' theorem level, KT). In the second step, Hartree-Fock calculations were performed for the core ionized states in order to account for the relaxation effects after ionization, i.e. for the "final state" effects (DeltaSCF level). Scalar relativistic corrections and spin-orbit coupling were included in a "spin-orbit-coupling configuration interaction" (SOC-CI) treatment both at the KT and DeltaSCF levels. In all Zn oxo compounds (Zn(4)O(formate)(6), Zn(4)O(acetate)(6) and several ZnO cubanes) small negative initial state shifts between -1.0 and 0.0 eV (relative to the free Zn atom) were found which are caused by the negative charges at the surrounding O atoms. The relaxation effects vary between -1.0 and -0.5 eV, such that the calculated total shifts are moderately negative (-1.5 to -0.5 eV). Embedded ZnO clusters of increasing size, ranging from Zn(13)O(4) to Zn(69)O(38), were used as models for bulk ZnO, the Zn 2s and 2p core level shifts calculated for these clusters being extrapolated to infinite cluster size. The calculations show that bulk ZnO has a rather large negative initial state shift of -2.1 +/- 0.1 eV, due to the Madelung potential at the Zn atom, and a comparatively small relaxation contribution of -1.0 +/- 0.1 eV. This yields a total shift of -3.1 +/- 0.2 eV (both for 2s and 2p, relative to atomic Zn), which is in very good agreement with experiment, -2.9 +/- 0.2 eV. The surprising experimental observation that the Zn 2s and 2p XPS peak positions are nearly identical in Zn metal and ZnO is explained by the fact that the sum of initial and final state effects is accidentally the same for the two systems though the individual contributions differ quite significantly: the initial and final state shifts amount to +2.4 and -5.1 eV for Zn metal vs.-2.1 and -1.0 eV for ZnO.     

Soft X-ray characterization of Zn(1-x)Sn(x)O(y) electronic structure for thin film photovoltaics

Zinc tin oxide (Zn(1-x)Sn(x)O(y)) has been proposed as an alternative buffer layer material to the toxic, and light narrow-bandgap CdS layer in CuIn(1-x),Ga(x)Se(2) thin film solar cell modules. In this present study, synchrotron-based soft X-ray absorption and emission spectroscopies have been employed to probe the densities of states of intrinsic ZnO, Zn(1-x)Sn(x)O(y) and SnO(x) thin films grown by atomic layer deposition. A distinct variation in the bandgap is observed with increasing Sn concentration, which has been confirmed independently by combined ellipsometry-reflectometry measurements. These data correlate directly to the open circuit potentials of corresponding solar cells, indicating that the buffer layer composition is associated with a modification of the band discontinuity at the CIGS interface. Resonantly excited emission spectra, which express the admixture of unoccupied O 2p with Zn 3d, 4s, and 4p states, reveal a strong suppression in the hybridization between the O 2p conduction band and the Zn 3d valence band with increasing Sn concentration.     

Ab initio calculations of the O1s XPS spectra of ZnO and Zn oxo compounds

O1s core level binding energies of oxygen atoms in bulk ZnO, at different ZnO surfaces, and in some Zn oxo compounds were calculated by means of wave function based quantum chemical ab initio methods. Initial and final state effects were obtained by Koopmans' theorem and at the DeltaSCF level, respectively. After correction for scalar relativistic effects and electron correlation, the calculated XPS peak positions are in excellent agreement with the available experimental data for all systems included in the present study. The O1s core level shifts between an isolated H2O molecule and the Zn oxo compounds or ZnO, as well as between oxygen atoms in bulk ZnO and at various ZnO surfaces, can be understood by means of Madelung potentials and electronic relaxation or screening. XPS spectra were calculated for various cluster models which are designed to describe different possibilities of stabilizing the polar O-terminated ZnO(0001) surface by the adsorption of H atoms. The experimental spectra are only compatible with the theoretical results for the fully hydroxylated H-ZnO(0001) surface exhibiting a (1x1) surface structure.     

Determination of ZnO(0001) surface termination by x‐ray photoelectron spectroscopy at photoemission angles of 0° and 70°

We present an XPS method to determine the termination of the ZnO(0001) surface. By measuring O 1s and Zn 2p_3/2 core‐level x‐ray photoelectron spectra at photoemission angles of 0° and 70° and comparing the intensity ratio (I_O1s/I_Zn2p3)_θ=0/(I_O1s/I_Zn2p3)_θ=70, the Zn and O termination can be distinguished. Calculations show that these two terminations have intensity ratios differing by ～17%. This difference is not affected by a contamination layer provided that the contamination layer thickness is the same for these two differently terminated surfaces. Although this determination method prefers a clean ZnO(0001) surface (in situ measurement), it seems also feasible for surfaces with known contamination layer thickness (ex situ measurement). We have measured ex situ ZnO(0001)‐Zn, ZnO(000&1macr;)‐O single crystals and an epitaxial ZnO film deposited on Al₂O₃(0001). The measured intensity ratios of the first two samples agree with the calculated values for a 0.2 and 0.26 nm contamination layer, respectively. The intensity ratio and the O 1s contamination component intensity of the epitaxial ZnO film are close to those of the ZnO(0001)‐Zn single crystal thus pointing at Zn termination of the film. Copyright © 2004 John Wiley & Sons, Ltd.     

纳米V2O5／ZnO光催化剂对壬基酚聚氧乙烯醚降解的催化活性

采用氨浸法制备了不同V2O5含量的纳米V2O5/ZnO光催化剂,并用X射线衍射、比表面积测定、透射电镜、X射线光电子能谱和漫反射紫外-可见光谱测定了催化剂的晶型、比表面积、形貌尺寸、表面组成和光谱特征.以壬基酚聚氧乙烯醚(NPE-10)为模型污染物,分别在紫外光和可见光照射下考察了光催化剂的催化活性.结果表明,随着V2O5含量的增加,V2O5/ZnO的粒径逐渐减小,比表面积逐渐增大.与纳米ZnO样品相比,V2O5/ZnO中V2p的结合能减小,而Zn2p和O1s的结合能增大,V2O5/ZnO表面的羟基氧和吸附氧含量增加.n(V)/n(Zn)=2·5%的V2O5/ZnO光催化剂样品的催化活性最高(在紫外光和可见光照射3h后,NPE-10降解率分别约为79%和62%).     

CO2选择性氧化甲烷制C2烃催化剂La2O3/ZnO的氧化还原和CO2吸附性能

Ｌａ２Ｏ３／ＺｎＯ催化剂体系在以二氧化碳作为氧化剂的甲烷氧化偶联反应中具有很高的Ｃ２烃选择性和稳定性．采用ＣＯ２－ＴＰＤ－ＭＳ和ＴＰＲ技术考察了Ｌａ２Ｏ３／ＺｎＯ对ＣＯ２的吸附性质及其氧化还原行为．结果表明：（１）Ｌａ２Ｏ３／ＺｎＯ催化剂体系存在着强、弱两种碱中心，其中弱碱中心数量随样品中Ｌａ２Ｏ３含量增加而减少，强碱中心强度随样品中Ｌａ２Ｏ３含量增加而增强．（２）由于组分相互作用，高温下，Ｌａ２Ｏ３／ＺｎＯ易产生晶格氧空位，使之对ＣＯ２的吸附增强，吸附后的ＣＯ２与晶格氧作用形成立方晶型Ｌａ２Ｏ２ＣＯ３．（３）Ｌａ２Ｏ３／ＺｎＯ表面的Ｌａ３＋和Ｚｎ２＋可以部分被还原，由于组分间的相互作用，使得二者的还原都较单一组分存在时更难．（４）Ｈ２－ＣＯ２－Ｈ２氧化还原循环实验表明，Ｌａ２Ｏ３／ＺｎＯ表面被部分还原后，ＣＯ２可以将部分被还原的表面再氧化．在此基础上对Ｌａ２Ｏ３／ＺｎＯ催化剂上甲烷与ＣＯ２转化为Ｃ２烃的机制也进行了讨论．     

助剂前体ZnSO_4浓度对苯选择加氢制环己烯Ru-Zn催化剂性能的影响

共沉淀法制备了Ru-Zn催化剂,在ZrO_2作分散剂下考察了助剂前体ZnSO_4浓度对苯选择加氢制环己烯Ru-Zn催化剂性能的影响.并用X-射线衍射(XRD)、X-射线荧光光谱(XRF)、N_2-物理吸附、透射电镜(TEM)和X-射线光电子能谱(XPS)等手段对催化剂进行了表征.结果表明,当ZnSO_4前体浓度低于0.10 mol/L时,Ru-Zn催化剂中Zn以ZnO形式存在,在加氢过程中ZnO可以与反应修饰剂ZnSO_4反应生成(Zn( OH)_2)_3(ZnSO_4)(H_2O)_3盐.继续增加ZnSO_4前体浓度,催化剂中Zn以ZnO和NaZn_4(SO_4)(Cl)(OH)_6·6H_2O盐存在,在加氢过程中ZnO和NaZn_4(SO_4)(Cl)(OH)_6·6H_2O盐可以与反应修饰剂ZnSO_4反应生成(Zn( OH)_2)_3(ZnSO_4)(H_2O)_5.(Zn( OH)_2)_3(ZnSO_4)(H_2O)_x(x=3或5)盐的Zn~(2+)可以转移金属Ru的部分电子.因此,随ZnSO_4前体浓度的增加,(Zn( OH)_2)_3(ZnSO_4)(H_2O)_x的量逐渐增加,金属Ru失电子越多,催化剂活性越低,环己烯选择性越高.0.08 mol/L ZnSO_4前体制备Ru-Zn催化剂给出了59.1%的环己烯收率,而且该催化剂具有良好的重复使用性能和稳定性.     

Density functional theory investigation of structure,stability, and glycerol/hydrogen adsorption on Cu,Cu?Zn,and Cu?ZnO clusters

Extensive density functional theory calculations are performed to analyze the structure and activity of Cu and Cu Zn/Cu ZnO clusters containing up to 10 Cu/Zn atoms. The minimum-energy structures of Cu Zn and Cu ZnO clusters are found by doping minimum-energy pure Cu clusters with Zn atom(s) and ZnO molecule(s), respectively, followed by energy minimization of the resultant clusters. Odd-even alteration in properties that determine cluster stability/activity is observed with cluster size, which may be attributed to the presence/absence of unpaired electrons. The difference in behavior between Zn/ZnO doping can be interpreted in terms of charge transfer between atoms. Charge transfers from Zn to Cu in the Cu Zn clusters and from Cu and Zn atoms to O atom in Cu-ZnO clusters, which implies that the Cu atom acts as an electron acceptor in the Cu Zn clusters but not in the Cu ZnO clusters. Finally, the adsorption energies of glycerol and hydrogen on Cu Zn/Cu ZnO clusters are computed in the context of the use of Cu Zn/Cu ZnO catalysts in glycerol hydrogenolysis. Glycerol adsorption is generally found to be more energetically favorable than hydrogen adsorption. Dual-site glycerol adsorption is also observed in some of the planar clusters. Fundamental insights obtained in this study can be useful in the design of Cu Zn/Cu ZnO catalysts.     

Zn adsorption on Pd(111): ZnO and PdZn alloy formation

The adsorption and thermal desorption of Zn and ZnO on Pd(111) was studied in the temperature range between 300 and 1300 K with TDS, LEED, and CO adsorption measurements. At temperatures below 400 K, multilayer growth of Zn metal on the Pd(111) surface takes place. At a coverage of 0.75 ML of Zn, a p(2 x 2)-3Zn LEED structure is observed. Increasing the coverage to 3 ML results in a (1 x 1) LEED pattern arising from an ordered Zn multilayer on Pd(111). Thermal desorption of the Zn multilayer state leads to two distinct Zn desorption peaks: a low-temperature desorption peak (400-650 K) arising from upper Zn layers and a second peak (800-1300 K) originating from the residual 1 ML Zn overlayer, which is more strongly bound to the Pd(111) surface and blocks CO adsorption completely. Above 650 K, this Zn adlayer diffuses into the subsurface region and the surface is depleted in Zn, as can be deduced from an increased amount of CO adsorption sites. Deposition of >3 ML of Zn at 750 K leads to the formation of a well-ordered Pd-Zn alloy exhibiting a (6 x 4 square root 3/3)rect. LEED structure. CO adsorption measurements on this surface alloy indicate a high Pd surface concentration and a strong reduction of the CO adsorption energy. Deposition of Zn at T > 373 K in 10(-6) mbar of O2 leads to the formation of an epitaxial (6 x 6) ZnO overlayer on Pd(111). Dissociative desorption of ZnO from this overlayer occurs quantitatively both with respect to Zn and O2 above 750 K, providing a reliable calibration for both ZnO, Zn, and oxygen coverage.     

Fe3+改性纳米ZnO光催化降解壬基酚聚氧乙烯醚

采用氨浸法制备了不同Fe3 含量的Fe3 /ZnO光催化剂,并用X射线衍射、N2吸附、X射线光电子能谱和紫外-可见漫反射光谱对纳米Fe3 /ZnO进行了表征.以壬基酚聚氧乙烯醚(NPE-10)为模型污染物,分别在紫外光和可见光下考察了纳米Fe3 /ZnO的光催化活性.结果表明,该方法能成功地将Fe掺杂到ZnO晶体上,且随着Fe3 添加量的增加,ZnO的晶粒尺寸逐渐减小,比表面积逐渐增大.与纳米ZnO样品相比,Fe3 /ZnO中Fe2p结合能减小,而Zn2p和O1s结合能增大,ZnO表面的羟基氧和吸附氧含量增加,光催化活性提高.当Fe3 的添加量大于0.5%时,Fe3 /ZnO样品的吸收光谱发生红移,在可见光区出现吸收.光催化降解结果显示,0.5?3 /ZnO样品的光催化活性最高,在紫外光和可见光照射3h后对NPE-10的降解率分别比纯ZnO提高18%和69%.