Pt／钇稳定氧化锆固体电解质在高温下的电化学性质

用交流阻抗技术研究了二电极、三电极Ｐｔ／钇稳定氧化锆（简称ＹＳＺ）高温固体电化学体系．开路电位下，Ｐｔ／ＹＳＺ体系只有一个阻抗半圆，对应于电极体系的电化学活化控制过程，极化电阻随温度变化的表观活化能为１７１．５ｋＪ／ｍｏｌ．Ｐｔ／ＹＳＺ界面的双电层电容约为３００μＦ／ｃｍ２．阳极极化下，交流阻抗极化电阻显著减小；阴极极化下，极化电阻反而增大，并出现浓差控制现象．     

Pt／YSZ固体电解质界面的电化学动力学研究

用循环伏安，线性扫描等电化学方法研究Ｐｔ／ＹＳＺ固体电解质界面的电化学行为，发现氧在Ｐｔ上的电化学吸附过程是Ｔｅｍｋｉｎ吸附过程，吸附量随时间对数增加，吸附氧的阴极还原是不可逆的过程，通过研究获得吸附氧阴极还原过电荷传递系数，Ｔｅｍｋｉｎ系数等重要参数。     

金属基上以YSZ为过渡层的YBCO薄膜的微观结构

采用透射电子显微术（ＴＥＭ），研究了用磁控溅射技术在柔性金属基体上制备的、钇稳定的ＺｒＯ２（ＹＳＺ）为过镀层的ＹＢａ２Ｃｕ３Ｏ７－ｙ（ＹＢＣＯ）薄膜的横断面结构。所得ＹＢＣＯ膜的超导临界转变温度Ｔｃ为９１Ｋ，临界电流密度Ｊｃ＝２×１０３Ａ／ｃｍ２（７７Ｋ，０Ｔ）。基体为Ｎｉ基合金（ＨａｓｔｅｌｏｙＣ）。ＹＳＺ层为致密、均匀的细晶组织，约１２μｍ厚，具有织构取向，并与基体紧密连接。ＹＢＣＯ层的厚度不均匀，约５００ｎｍ；ＹＢＣＯ／ＹＳＺ界面有时连接较差，在该界面上有杂质出现，杂质有可能引发裂纹。     

硼掺杂多晶金刚石薄膜电极的电化学特性

用循环伏安法和恒电位法研究了硼掺杂多晶金刚石薄膜电极（ＤＦＥ）的若干电化学特性。电极面积４×４ｍｍ＾２。在０．１ｍｏｌ／Ｌ ＫＣｌ，ＮａＮＯ３，ＮａＯＨ和ＫＨ２ＰＯ４＋Ｎａ２ＨＰＯ４（ｐＨ＝６．８６）电解质溶液中电势窗口均为－５００￣＋８００ｍＶ；而在０．１ｍｏｌ／Ｌ ＨＣｌ和Ｈ２ＳＯ４溶液中电势窗口为－２００￣＋１１００ｍＶ．Ｋ３Ｆｅ（ＣＮ）６的氧化峰电位为＋５００ｍＶ，与Ｐｔ电极测量相同；校正     

ZSM－5沸石中V的还原性能

用ＴＰＲ并结合ＸＲＤ、ＥＳＲ和ＸＰＳ等测试手段研究了Ｖ（Ⅳ，Ⅴ）－ＺＳＭ－５、Ｖ２Ｏ５－／ＺＳＭ－５（分别用浸渍法和机械混合法制备）及Ｖ２Ｏ５样品的还原性能，获得了还原过程中物相及钒离子价态变化的信息，发现分散在分子筛表面上的Ｖ（Ⅴ）还原温度比Ｖ２Ｏ５低，而位于ＺＳＭ－５骨架上的Ｖ（Ⅴ）却比Ｖ２Ｏ５更难还原。高于１２００Ｋ骨架Ｖ才开始还原；高于１３７０Ｋ，Ｖ－ＺＳＭ－５分子筛开始解体并转变成方英石结构，从骨架中析出的Ｖ完全还原成低价态。     

甲烷与PtCl2（H2O）x（x=0,1,2）的配合物结构的从头算研究

本文用量子化学从头算方法研究了甲烷与配位不饱和ＰｔＣｌ２（Ｈ２Ｏ）ｘ（ｘ＝０，１，２）形成的σ配合物的结构和性质。通过ＲＨＦ／Ｌａｎ１２ＤＺ和ＭＰ２／Ｌａｎ１２ＤＺ水平计算讨论了溶剂Ｈ２Ｏ分子与位的影响。在ＲＨＦ／Ｌａｎ１２ＤＺ级别上有４个稳定的（ＣＨ４）ＰｔＣｌ２配合物，分别属于η＾３，η＾２，η＾３，并都具有Ｃｓ对称性。根据能量和结构分析，η＾１配合物是进一步氧化加成反应的可能的起始物。     

YBCO／CeO2／Si多层膜超导材料的分析电镜研究

在具有ＣｅＯ２隔离层的Ｓｉ基片上获得了较高质量的ＹＢａ２Ｃｕ３Ｏ７－ｘ（ＹＢＣＯ）高温超导薄膜。在零磁场下，７７Ｋ时其临界电流密度达到１×１０６Ａ／ｃｍ２。研究发现，ＹＢＣＯ的（００１）面平行于Ｓｉ基片的（１００）面，而ＣｅＯ２过渡层由许多约４０ｎｍ×１００ｎｍ的细小ＣｅＯ２晶粒组成，其取向呈散乱分布。尽管ＣｅＯ２和Ｓｉ之间的晶格错配很小（约０．４％），ＣｅＯ２却不能在Ｓｉ上外延生长，而ＹＢＣＯ却能在取向凌乱的ＣｅＯ２上形成［００１］择优取向。ＣｅＯ２和Ｓｉ的界面处有一层极薄的过度层。ＹＢＣＯ和ＣｅＯ２界面存在Ｙ２ＢａＣｕＯ５（２１１相）。在ＹＢＣＯ薄膜中观察到有与１２３相混生的２４８相。     

毛细管区带电泳法测定甲氧苄胺嘧啶和磺胺甲基异噁唑的离解常数及其在复方新诺明中的含量

报道了利用 ３０ ｍｍｌ／Ｌ ＨＡｃ－ＮａＡｃ为缓冲液测定复方新诺明中甲氧苄胺嘧啶（ＴＭＰ）和磺胺甲基异噁唑（ＳＭＺ）的离解常数及含量的毛细管区带电泳（ＣＺＥ）方法。该方法具有简便、快速、准确等特点。测得ＴＭＰ和ＳＭＺ的ｐＫａ分别为６．６０和５．９０。其平均回收率分别为１０１．５％和９９．６％,最低检出限为０．４８ ｍｇ／Ｌ和０．０２８ ｍｇ／Ｌ,ＲＳＤ为１．２６％和１．１２％。     

SYNTHESIS OF 4－S－（5″－ALKYL－4″－AMINO－1″，2″，4″－TRIAZOLE－3″－YL）－4－DEOXY－4′－DEMETHYL－EPIPODOPHYLLOTOXIN ANALOGUES

ＳＹＮＴＨＥＳＩＳＯＦ４－Ｓ－（５″－ＡＬＫＹＬ－４″－ＡＭＩＮＯ－１″，２″，４″－ＴＲＩＡＺＯＬＥ－３″－ＹＬ）－４－ＤＥＯＸＹ－４′－ＤＥＭＥＴＨＹＬ－ＥＰＩＰＯＤＯＰＨＹＬＬＯＴＯＸＩＮＡＮＡＬＯＧＵＥＳ￥ＫｕａｎＫｅＬＵ；ＦａｎｇＭｉｎＬＩ...     

La0.8Sr0.2MnO3/YSZ电极氧电化学还原反应动力学

用线性极化、循环伏安、电位阶跃等方法详细研究了Ｌａ０．８Ｓｒ０．２ＭｎＯ３／ＹＳＺ高温电极上进行的氧化学还原反应。实验结果表明，该反应存在两条路径：低温下氧还原反应主要发生在气相－ＬＳＭ电极－ＹＳＺ电解质接触的三相界面（ＴＰＢ），速度控制步骤为氧原子在ＬＳＭ表面的浓差扩散，高温下由于氧空位在ＬＳＭ表面的形成，氧还原反应区扩展至ＬＳＭ电极表面，速度控制步骤为氧的电荷转移反应，实验同时发现：氧空位的形     

Kinetics of oxygen exchange over CeO2-ZrO2 fluorite-based catalysts

The kinetics of 18O/16O isotopic exchange over CeO2-ZrO2-La2O3 and Pt/CeO2-ZrO2 catalysts have been investigated under the conditions of dynamic adsorption-desorption equilibrium at atmospheric pressure and a temperature range of 650-850 degrees C. The rates of oxygen adsorption-desorption on Pt sites, support surface, oxygen transfer (spillover) from Pt to the support as well as the amount of oxygen accumulated in the oxide bulk, and oxygen diffusion coefficient were estimated. The nanocrystalline structure of lanthana-doped ceria-zirconia prepared via the Pechini route with a developed network of domain boundaries and specific defects guarantees a high oxygen mobility in the oxide bulk (D = (1.5 / 2.0).10-18 m2 s-1 at 650 degrees C) and allows accumulation of over-stoichiometric/excess oxygen. For Pt/CeO2-ZrO2, oxygen transfer from Pt to support (characteristic time < 10-2 s) was shown to be responsible for the fast exchange between the gas-phase oxygen and oxygen adsorbed on the mixed oxide surface. The rate of direct exchange between the gas phase and surface oxygen is increased as well due to the increased concentration (up to 2 monolayers) of surface/near subsurface oxygen species accumulated on the oxygen vacancies (originated from the incorporation of highly dispersed Pt atoms). The characteristic time of diffusion of the oxygen localized in the subsurface layers is about 1 s. The overall quantity of over-stoichiometric oxygen and/or hydroxyl groups accumulated in the bulk can reach the equivalent of 10 monolayers, and characteristic time of oxygen diffusion within the bulk is about 20 s. All these kinetic data are required for the further step of modeling partial oxidation of hydrocarbons under steady- and unsteady-state conditions.     

Electron-stimulated sputtering of thin amorphous solid water films on Pt(111)

The electron-stimulated sputtering of thin amorphous solid water films deposited on Pt(111) is investigated. The sputtering appears to be dominated by two processes: (1) electron-stimulated desorption of water molecules and (2) electron-stimulated reactions leading to the production of molecular hydrogen and molecular oxygen. The electron-stimulated desorption of water increases monotonically with increasing film thickness. In contrast, the total sputtering--which includes all electron-stimulated reaction channels--is maximized for films of intermediate thickness. The sputtering yield versus thickness indicates that erosion of the film occurs due to reactions at both the water/vacuum interface and the Pt/water interface. Experiments with layered films of D2O and H2O demonstrate significant loss of hydrogen due to reactions at the Pt/water interface. The electron-stimulated sputtering is independent of temperature below approximately 80 K and increases rapidly at higher temperatures.     

Cation self-diffusion in LaCoO(3) and La(2)CoO(4) studied by diffusion couple experiments

Reaction kinetics between dense, polycrystalline pellets of La2O3 and CoO were investigated at temperatures of 1370-1673 K and oxygen partial pressures of 40 Pa - 50 kPa. At high oxygen partial pressures, single phase LaCoO3 was formed. The growth of the LaCoO3 phase followed the parabolic rate law. The location of Pt markers demonstrated that diffusion of Co3+ cations in LaCoO3 dominated over diffusion of La3+. The diffusion coefficient of Co3+ was determined from the parabolic rate constant, and an activation energy of (250 +/- 10) kJ mol-1 was found. The diffusion coefficient of Co3+ in LaCoO3 decreased with decreasing oxygen partial pressure. At the lowest oxygen partial pressure investigated, two product phases, LaCoO3 and La2CoO4, were observed. The diffusion coefficient of Co cations in La2CoO4 was estimated. Results were discussed in relation to cation diffusion in other LnBO3 oxides (B = Cr3+, Mn3+, Fe3+). A correlation between diffusion of the B cation and the melting point was found for LnBO3 materials.     

Oxygen adsorption on Pt/Ru(0001) layers

Chemical properties of epitaxially grown bimetallic layers may deviate substantially from the behavior of their constituents. Strain in conjunction with electronic effects due to the nearby interface represent the dominant contribution to this modification. One of the simplest surface processes to characterize reactivity of these substrates is the dissociative adsorption of an incoming homo-nuclear diatomic molecule. In this study, the adsorption of O(2) on various epitaxially grown Pt films on Ru(0001) has been investigated using infrared absorption spectroscopy and thermal desorption spectroscopy. Pt/Ru(0001) has been chosen as a model system to analyze the individual influences of lateral strain and of the residual substrate interaction on the energetics of a dissociative adsorption system. It is found that adsorption and dissociative sticking depends dramatically on Pt film thickness. Even though oxygen adsorption proceeds in a straightforward manner on Pt(111) and Ru(0001), molecular chemisorption of oxygen on Pt/Ru(0001) is entirely suppressed for the Pt/Ru(0001) monolayer. For two Pt layers chemisorbed molecular oxygen on Pt terraces is produced, albeit at a very slow rate; however, no (thermally induced) dissociation occurs. Only for Pt layer thicknesses N(Pt) ≥ 3 sticking gradually speeds up and annealing leads to dissociation of O(2), thereby approaching the behavior for oxygen adsorption on genuine Pt(111). For Pt monolayer films a novel state of chemisorbed O(2), most likely located at step edges of Pt monolayer islands is identified. This state is readily populated which precludes an activation barrier towards adsorption, in contrast to adsorption on terrace sites of the Pt/Ru(0001) monolayer.     

Surface tension and its temperature coefficient of molten tin determined with the sessile drop method at different oxygen partial pressures

The surface tension of molten tin has been determined by the sessile drop method at temperatures ranging from 523 to 1033 K and in the oxygen partial pressure (P(O(2))) range from 2.85 x 10(-19) to 8.56 x 10(-6) MPa, and its dependence on temperature and oxygen partial pressure has been analyzed. At P(O(2))=2.85 x 10(-19) and 1.06 x 10(-15) MPa, the surface tension decreases linearly with the increase of temperature and its temperature coefficients are -0.151 and -0.094 mN m(-1) K(-1), respectively. However, at high P(O(2)) (3.17 x 10(-10), 8.56 x 10(-6) MPa), the surface tension increases with the temperature near the melting point (505 K) and decreases above 723 K. The surface tension decrease with increasing P(O(2)) is much larger near the melting point than at temperatures above 823 K. The contact angle between the molten tin and the alumina substrate is 158-173 degrees, and the wettability is poor.     

Electron-stimulated production of molecular oxygen in amorphous solid water on Pt111: precursor transport through the hydrogen bonding network

The low-energy, electron-stimulated production of molecular oxygen from thin amorphous solid water (ASW) films adsorbed on Pt(111) is investigated. For ASW coverages less than approximately 60 ML, the O(2) electron-stimulated desorption (ESD) yield depends on coverage in a manner that is very similar to the H(2) ESD yield. In particular, both the O(2) and H(2) ESD yields have a pronounced maximum at approximately 20 ML due to reactions at the Pt/water interface. The O(2) yield is dose dependent and several precursors (OH, H(2)O(2), and HO(2)) are involved in the O(2) production. Layered films of H(2) (16)O and H(2) (18)O are used to profile the spatial distribution of the electron-stimulated reactions leading to oxygen within the water films. Independent of the ASW film thickness, the final reactions leading to O(2) occur at or near the ASW/vacuum interface. However, for ASW coverages less than approximately 40 ML, the results indicate that dissociation of water molecules at the ASW/Pt interface contributes to the O(2) production at the ASW/vacuum interface presumably via the generation of OH radicals near the Pt substrate. The OH (or possibly OH(-)) segregates to the vacuum interface where it contributes to the reactions at that interface. The electron-stimulated migration of precursors to the vacuum interface occurs via transport through the hydrogen bond network of the ASW without motion of the oxygen atoms. A simple kinetic model of the nonthermal reactions leading to O(2), which was previously used to account for reactions in thick ASW films, is modified to account for the electron-stimulated migration of precursors.     

In situ ATR-IR spectroscopic and reaction kinetics studies of water-gas shift and methanol reforming on Pt/Al2O3 catalysts in vapor and liquid phases

Reaction kinetics measurements of the water-gas shift reaction were carried out at 373 K on Pt/Al2O3 in vapor phase to investigate the effects of CO, H2, and H2O partial pressures. Results of in situ ATR-IR studies conducted in vapor phase under similar conditions suggest that the Pt surface coverage by adsorbed CO is high (approximately 90% of the saturation coverage), leading to a negligible effect of the CO pressures on the rate of reaction. The negative reaction order with respect to the H2 pressure is caused by the increased coverage of adsorbed H atoms, and the fractional positive order with respect to the water pressure is consistent with non-equilibrated H2O dissociation on Pt. Results of in situ ATR-IR studies carried out at 373 K show that the presence of liquid water leads to a slight decrease in the Pt surface coverage by adsorbed CO (approximately 80% of the saturation coverage) when the CO partial pressure is the same as in the vapor-phase studies. The rate of the WGS reaction in the presence of liquid water is comparable to the rate under complete vaporization conditions when other factors (such as CO partial pressure) are held constant. Reaction kinetics measurements of methanol reforming were carried out at 423 K over a total pressure range of 1.36-5.84 bar. In situ ATR-IR studies were conducted at 423 K to determine the Pt surface coverage by adsorbed CO in completely vaporized methanol feeds and in aqueous methanol solutions. The decomposition of methanol is found to be slower during the reforming of methanol in liquid phase than in vapor phase, which leads to a lower rate of hydrogen production in liquid phase (0.08 min(-1) at 4.88 bar) than in vapor phase (0.23 min(-1) at 4.46 bar). The lower reaction order with respect to methanol concentration observed for vapor-phase versus liquid-phase methanol reforming (0.2 versus 0.8, respectively) is due to the higher extent of CO poisoning on Pt for reforming in vapor phase than in liquid phase, based on the higher coverage by adsorbed CO observed in completely vaporized methanol feeds (55-60% of the saturation coverage) than in aqueous methanol feed solutions (29-40% of the saturation coverage).     

Quenching of I(2P1/2) by NO2, N2O4, and N2O

Quenching of excited iodine atoms (I(5p5, 2P1/2)) by nitrogen oxides are processes of relevance to discharge-driven oxygen iodine lasers. Rate constants at ambient and elevated temperatures (293-380 K) for quenching of I(2P1/2) atoms by NO2, N2O4, and N2O have been measured using time-resolved I(2P1/2) --> I(2P3/2) 1315 nm emission. The excited atoms were generated by pulsed laser photodissociation of CF3I at 248 nm. The rate constants for I(2P1/2) quenching by NO2 and N2O were found to be independent of temperature over the range examined with average values of (2.9 +/- 0.3) x 10(-15) and (1.4 +/- 0.1) x 10(-15) cm3 s(-1), respectively. The rate constant for quenching of I(2P1/2) by N2O4 was found to be (3.5 +/- 0.5) x 10(-13) cm3 s(-1) at ambient temperature.     

NO2在Ag/Pt(110)双金属表面上的吸附和分解

利用俄歇电子能谱(AES)和程序升温脱附谱(TDS)研究了NO₂在Ag/Pt(110)双金属表面的吸附和分解.室温下NO₂ 在Ag/Pt(110)双金属表面发生解离吸附, 生成NO(ads)和O(ads)表面吸附物种. 在升温过程中NO(ads)物种发生脱附或者进一步分解. 500 K时NO₂在Ag/Pt(110)双金属表面发生解离吸附生成O(ads)表面吸附物种. Pt 向Ag传递电子, 从而削弱Pt－O键的强度, 降低O(ads)从Pt 表面的并合脱附温度. 发现能够形成具有稳定组成的Ag/Pt(110)合金结构, 其表现出与Pt(110)-(1×2)相似的解离吸附NO₂能力, 但与O(ads)的结合明显弱于Pt(110)-(1×2). 该AgPt(110)合金结构是可能的低温催化直接分解氮氧化物活性结构.