氧化铁还原率及金属化率的测量新方法

用H₂及CO还原氧化铁过程中,使用了X-ray粉末衍射和化学分析方法确定了氧化铁及金属铁的定量分析关系。铁素体(α_Fe)、奥氏体(γ_Fe)、碳化铁(Fe₃C)、磁铁矿(Fe₃O₄)、赤铁矿(Fe₂O₃)与浮氏体(Fe_0.947O)的摩尔强度定量关系的系数分别为0.56,0.56,0.52,0.87和2.57。通过这些系数,可以计算出氧化铁的金属化率和还原率。     

桑色素修饰金纳米粒子自组装膜的制备及其性能研究

采用水相硅烷化方法,将γ-氨基丙基三乙氧基硅烷[H₂N(CH₂)₃Si(OC₂H₅)₃](APES)组装在石英表面,在基底表面修饰上氨基为末端的单层膜,并进一步在这种功能化的单层膜基底上组装金纳米粒子得到金纳米粒子/APES/石英的纳米复合结构。以制备的金纳米粒子自组装膜修饰石英为基底及DL-半胱胺酸为中介,利用桑色素(Morin)和DL-半胱胺酸的化学吸附作用,将桑色素间接组装在金纳米粒子自组装膜修饰石英基底表面,所构建的桑色素修饰金纳米粒子自组装膜对三苯基锡有灵敏的荧光识别作用。文章着重研究了桑色素修饰金纳米粒子自组装膜的制备以及组装条件对其荧光行为的影响,探讨了膜的响应特性及响应机理。     

不同因素影响下Fe(Ⅲ)水解中和法制备FeOOH矿相的光谱分析

羟基氧化铁(FeOOH)作为重金属等污染物的吸附材料倍受关注,但不同因素作用下形成的FeOOH产物矿相、结构性质的差异及其对环境功能的影响,却少有报道。采用X射线衍射仪,红外光谱仪,扫描电子显微镜和激光粒度分析仪,系统考察了Fe(Ⅲ)溶液水解中和形成FeOOH时,不同作用因素如铁盐种类、pH和温度等对产物矿相的影响。结果表明,pH 8条件下,Fe(Ⅲ)溶液水解产物均为二线水铁矿(Fe₅HO₈·4H₂O);随着pH升高,Fe₅HO₈·4H₂O会向α-FeOOH相转化。Cl-和NO-₃离子的存在分别有利于β-FeOOH和α-FeOOH的形成;SO2-₄会阻碍Fe₅HO₈·4H₂O向α-FeOOH相转化;Fe2+存在时,会促进Fe₅HO₈·4H₂O向α-FeOOH相转化。加热陈化,可促进Fe₅HO₈·4H₂O转化为α-FeOOH,且利于良好结晶α-FeOOH的形成。但pH≤5,富含Cl-的Fe(Ⅲ)溶液加热水解利于β-FeOOH的生成。不同因素影响下形成的FeOOH,在矿相、表面基团、颗粒形貌和粒径大小上存在一定的差异。     

被动式FTIR遥感掺纳米材料固体推进剂的燃烧火焰温度

应用被动式遥感FTIR,分别对掺入纳米级金属氧化物、掺入同种材料普通金属氧化物及无掺入物的固体推进剂的燃烧火焰温度进行了测量。固体推进剂的主要成分为硝化棉和硝化甘油。掺加物分别为6 nm CuO,56 nm Fe₂O₃,16 nm NiO粒子及相应的普通金属氧化物。FTIR仪器分辨率为1 cm-1。利用燃烧产物中H₂O分子在2.75 μm处的基带发射光谱精细结构,根据分子转振光谱测温法,计算出燃烧火焰温度。结果表明,掺有纳米级CuO,Fe₂O₃和NiO粒子的固体推进剂的燃烧火焰温度分别为3 089,3 193和3 183 K,此温度与掺入同种材料的普通金属氧化物和无掺入物的固体推进剂的燃烧火焰温度无明显差别。     

表面修饰的钛酸钡的拉曼光谱

采用水热法制得表面包裹有十二烷基苯磺酸(DBS)和硬脂酸(St)的BaTiO₃纳米粒子，平均粒径均为60nm左右.拉曼光谱检测结果表明，样品的确为表面包裹有表面活性剂(DBS或St)的BaTiO₃纳米粒子集合体.与未包裹的相比，各光学声子模对应的拉曼振动模式峰均发生了蓝移.还发现不同的包裹体，所导致的蓝移值也不同.从纳米粒子的表面结构及包裹层的压力出发对此现象进行了定性解释和讨论. 关键词： 拉曼光谱 3纳米粒子')" href="#">DBS/ BaTiO₃纳米粒子 蓝移     

钢大气腐蚀锈层的红外、拉曼光谱研究

运用红外光谱、拉曼光谱分析的方法,对碳钢A₃和低合金钢10CrMoAl经青岛大气腐蚀的锈层样品,进行了比较测试,综合分析得出锈层中主要组成物相为α-Fe₂O₃,γ-FeOOH, α-FeOOH, δ-FeOOH,Fe₃O₄,以及各组成物相相对含量随腐蚀时间的变化情况。     

硼酸盐润滑油添加剂的摩擦化学机理研究

硼酸盐润滑油添加剂的摩擦磨损表面经小面积Ｘ射线光电子能谱（ＸＰＳ）和剖面ＸＰＳ分析发现，摩擦磨损表面生成了复杂的摩擦化学保护膜，该保护膜主要由吸附膜，沉积膜和摩擦化学产物组成，特别是ＢＮ化学物的生成，有利于改善其抗磨减摩性能。     

Si纳米量子点的LPCVD自组织化形成及其生长机理研究

采用低压化学汽相沉积(LPCVD)方法，依靠纯SiH₄气体分子的表面热分解反应， 在由Si—O—Si键和由Si—OH键终端的两种SiO₂表面上，自组织生长了Si纳米量子点. 实 验研究了所形成的Si纳米量子点密度随SiO₂表面的反应活性位置数、沉积温度以及反应气 压的变化关系. 依据LPCVD的表面热力学过程，定性地分析了Si纳米量子点的形成机理.研究结果对具有密度分布均匀和晶粒尺寸可控的Si纳米量子点的自组织生长，以及Si基新型量子电子器 关键词： Si纳米量子点 LPCVD 自组织化形成 生长机理     

高效稳定的CsPbBr3-Cs4PbBr6混合相钙钛矿纳米晶的制备及形成过程

通过配体后处理法向CsPbBr₃钙钛矿纳米晶中加入油胺-十四烷基膦酸(OLA-TDPA)的混合配体获得了CsPbBr₃-Cs₄PbBr₆混合材料.在最佳比例下(CsPbBr₃, TDPA与OLA的物质的量的比为1∶1∶15)制备的CsPbBr₃-Cs₄PbBr₆钙钛矿纳米晶混合相的光致发光量子产率可达78%,荧光寿命长达476 ns,且其在室温环境下保持稳定性至少25 d,在293 K和328 K之间的5个加热-冷却循环中具有良好的热稳定性.混合纳米晶的形成经历了表面钝化/溶解和重结晶两个阶段:在第1阶段(t≤1 h), OLA-TDPA混合配体形成了(RNH₃)₂PO₃X型配体与纳米晶表面发生配体交换,交换后的新配体能与纳米晶表面的Pb²⁺紧密的结合且含量较高,降低了纳米晶表面的缺陷态密度,提高了CsPbBr₃     

表面修饰纳米碳管复合二氧化硅凝胶玻璃的制备研究

采用羧基化、酰氯化和酰胺化等三步化学反应实现了r-氨基丙基三乙氧基硅烷(NH₂(CH₂)₃Si(OC₂H₅)₃,APTES)对纳米碳管(CNTs)的表面修饰。在此基础上,采用溶胶-凝胶工艺将其引入到二氧化硅凝胶玻璃中,并通过红外IR光谱、扫描电子显微镜SEM分析测试方法对所得样品的组成和结构进行表征。结果表明,经过一系列的化学处理,成功实现了CNTs与APTES的共价键合而达到表面修饰的效果。溶胶-凝胶过程中,先驱液中正硅酸乙酯(Si(OC₂H₅)₄,TEOS)、r-缩水甘油醚基丙基三甲氧基硅烷(CH₂OCHCH₂O(CH2)₃Si(OCH₃)₃,GPTMS)、CNTs-APTES分别发生水解,并经过共同聚合反应形成二氧化硅三维网络结构,而CNTs也借助于APTES而被化学键合到二氧化硅网络中,实现了在二氧化硅凝胶玻璃基质中的均匀分散,从根本上克服了CNTs在固相基质中团聚的问题。     

Oxidation kinetics of thin copper films and wetting behaviour of copper and Organic Solderability Preservatives (OSP) with lead-free solder

The oxide formation on thin copper films deposited on Si wafer was studied by XPS, SEM and Sequential Electrochemical Reduction Analysis SERA. The surfaces were oxidized in air with a reflow oven as used in electronic assembly at temperatures of 100 °C, 155 °C, 200 °C, 230 °C and 260 °C. The SERA analyses detected only the formation of Cu₂O but the XPS analysis done for the calibration of the SERA equipment proved also the presence of a CuO layer smaller than 2 nm above the Cu₂O oxide. The oxide growth follows a power-law dependence on time within this temperature range and an activation energy of 33.1 kJ/mol was obtained. The wettability of these surfaces was also determined by measuring the contact angle between solder and copper substrate after the soldering process. A correlation between oxide thickness and wetting angle was established. It was found that the wetting is acceptable only when the oxide thickness is smaller than 16 nm. An activation energy of 27 kJ/mol was acquired for the spreading of lead free solder on oxidized copper surfaces.From wetting tests on copper surfaces protected by Organic Solderability Preservatives (OSP), it was possible to calculate the activation energy for the thermal decomposition of these protective layers.     

Effect of surface roughness on the development of protective Al2O3 on Fe-10Al (at.%) alloys containing 0-10 at.% Cr

The effect of alloy surface roughness, achieved by different degrees of surface polishing, on the development of protective alumina layer on Fe-10 at.% Al alloys containing 0, 5, and 10 at.% Cr was investigated during oxidation at 1000 °C in 0.1 MPa oxygen. For alloys that are not strong Al₂O₃ formers (Fe-10Al and Fe-5Cr-10Al), the rougher surfaces increased Fe incorporation into the overall surface layer. On the Fe-10Al, more iron oxides were formed in a uniform layer of mixed aluminum- and iron-oxides since the layer was thicker. On the Fe-5Cr-10Al, more iron-rich nodules developed on an otherwise thin Al₂O₃ surface layer. These nodules nucleated preferentially along surface scratch marks but not on alloy grain boundaries. For the strong Al₂O₃-forming Fe-10Cr-10Al alloy, protective alumina surface layers were observed regardless of the surface roughness. These results indicate that the formation of a protective Al₂O₃ layer on Fe-Cr-Al surfaces is not dictated by Al diffusion to the surface. More cold-worked surfaces caused an enhanced Fe diffusion, hence produced more Fe-rich oxides during the early stage of oxidation.     

纳米Al2O3表面接枝修饰的XPS研究

在纳米Al2O3表面接枝聚缩醛可在粒子表面建立起空间位阻稳定层, 不但提高了纳米粒子的分散稳定性, 还可以增强纳米粒子与树脂基体的相容性. X射线光电子能谱(XPS)的分析结果表明, 经过聚缩醛接枝改性的纳米Al2O3的Al(2p)峰几乎消失, O(1s)峰也相应降低, 与之相对应的是C(1s)峰有了明显的增长, 对C(1s)峰精细扫描及分峰拟合表明, 纳米Al2O3表面碳元素中有61.92%属于接枝物聚缩醛的有机碳, 接枝物聚缩醛与纳米Al2O3形成了Al-O-C键, 两者产生化学结合. 同时对比XPS和热失重分析(TG)的数据结果, 可以推测聚缩醛主要分布在纳米Al2O3的表面, 而在体相中独立存在的概率较小.     

Surface chemistry of Fe2O3 nanoparticles on ultrathin oxide layers on Si and Ge

In this paper, we report on a comparative study of the effect of Fe₂O₃ nanoparticles (NP), introduced onto a thin oxide layer formed on silicon and germanium surfaces, on the thermal decomposition pathway of the individual oxide layers. On both the surfaces, NP of Fe₂O₃ undergo a reduction reaction through a bonding partner change reaction, where the oxygen atoms change from Fe to Si or Ge. On both the surfaces, annealing results in the conversion of the suboxide-like species to dioxide-like species (SiO_x to SiO₂ and GeO_x to GeO₂ respectively for Si and Ge surfaces), until the oxide layer decomposes following the desorption of the respective monoxide species (SiO and GeO). Both the Si and Ge corelevels show a larger chemical shift (4.1 and 3.51 eV in Si 2p and Ge 3d corelevels, respectively) for the as-prepared oxide samples with the NP, at room temperature compared to that without the NP (3.7 and 3.4 eV), indicating a catalytic enhancement of the dioxide formation. Selective formation of silicon oxides leads to encapsulation of the nanoparticles and acts like a protective layer, preventing the oxidation of Fe.     

Oxidation of iron: the relation between oxidation kinetics and oxide electronic structure

The test of the validity of the Fromhold-Cook theory of metal oxidation for the O2/Fe system in the tunnel regime is impeded by the growth of a passivating Fe2+/Fe3+ double layer at T150 degrees C, the thermionic emission of electrons is rate limiting for oxygen coverages larger than 13x10(15) atoms/cm(2).     

LEED-Auger characterization of GaAs during activation to negative electron affinity by the adsorption of Cs and O

A combination of low energy electron diffraction (LEED) and Auger electron spectroscopy (AES) has been used to study the formation of the negative electron affinity (NEA) condition on surfaces of p-type, degenerate, (100) and (111) GaAs. Activation to NEA is achieved by adsorbing Cs and O onto atomically clean GaAs in repetitive cycles of first Cs and then O. Before activation, the clean GaAs surfaces exhibit their characteristic LEED patterns. However, once obtained, there is no significant correlation between the quality of these LEED patterns and the final activation. The adsorption of both Cs and O during activation to NEA is amorphous. Auger measurements have shown that the first photoemission maximum occurs after the adsorption of about a half monolayer of Cs. The initial O adsorption occurs on the GaAs surface between the Cs atoms. The adsorbed O interacts strongly with Cs at any stage during the activation. Peak photosensitivities, after completion of the Cs and O adsorptions, were in the range 400 to 1100 $\text{μA}\text{lumen}$. The final activation does not correlate with the quantity of Cs and O on the surface. The temperature dependence of the photosensitivity of NEA GaAs (100) activated at ?170°C has a broad maximum at about ?50°C and a subsidiary maximum at about 160°C. In addition, the photoemission at ?170°C can be either increased or decreased by having heated the sample up to 200°C, even though no Cs or O desorption has taken place. These results can be traced to changes in work function rather than to changes in bulk properties. While the LEED patterns from clean GaAs show no structural changes with temperature, such changes are observed when Cs is on the surface. It is suggested that changes both in photoemission and in LEED patterns are due to the temperature-induced mobility of Cs on GaAs. An atomic model for the NEA surface is discussed in terms of a layer of Cs and O atoms about 10 Å thick on the GaAs.     

Epitaxial growth and magnetic exchange anisotropy in Fe3O4<Emphasis Type="Bold">/NiO bilayers grown on MgO(001) and Al</Emphasis>2O3(0001)

Epitaxial Fe3O4/NiO bilayers were epitaxially grown on MgO(001) and Al2O3(0001) substrates to investigate the influence of the fully spin compensated (001) and the non-compensated (111) NiO interface planes between the ferromagnetic (F) and antiferromagnetic (AF) layers on the AF/F exchange coupling. Bilayers of different magnetite thicknesses and constant NiO thickness were investigated. The structural characterizations indicate a perfect epitaxy of the two layers for the both growth directions in the two Fe3O4/NiO/MgO(001) and NiO/Fe3O4/Al2O3(0001) systems. An epitaxial ferrimagnetic (Ni,Fe)Fe2O4 phase is observed at the AF/F interface when the NiO oxide is grown on the top of the Fe3O4 layer while a perfectly flat AF/F interface is observed in the Fe3O4/NiO/MgO(001) system exhibiting only a very slight interdiffusion. Magnetic measurements indicate a relative strong bias at 300 K for the bilayers grown on Al2O3(0001), which decreases with the inverse of the ferrimagnetic layer thickness as theoretically expected. On the contrary, a zero exchange biasing is observed at 300 K for the bilayers grown on MgO(001).     

Fe2O3上AsH3催化氧化反应机理的理论研究

本文采用密度泛函理论方法研究了Fe₂O₃上AsH₃的催化氧化反应机理.该反应以Fe₂O₃中的两个Fe原子为不同的活性中心进行研究,每个活性中心均设计了3个步骤. AsH₃分子依次与3个O₂分子在催化剂上相互作用分别形成中间体H₃AsO₂、H₃AsO₄及最终产物H₃AsO₆.研究发现,当氧化反应发生在1号铁原子(Fe1)附近,其速度控制步骤活化自由能垒为49.99 kcal/mol;当氧化反应发生在2号铁原子(Fe2)附近,其活化自由能垒为21.20 kcal/mol,与直接氧化(50.14 kcal/mol)相比大大降低.可见AsH₃在Fe₂O₃上的催化氧化反应更易发生在Fe2附近.     

Laser interference metallurgy: A new method for periodic surface microstructure design on multilayered metallic thin films

Methods for micro- and nanostructuring are essential for functionalization of materials surfaces. In particular, photon-assisted methods for synthesis of functional surfaces have been intensively investigated in the last years. In this study, a new method for surface modification and production of long-range order periodical structures called “laser interference metallurgy” is explored. A metallic thin film sample consisting of three layers composed of Fe, Cu and Al (from top to bottom) on a glass substrate was irradiated with an interference pattern using a Nd:YAG laser (wavelength of 355 nm, 10 ns of pulse duration). For the interference pattern, a configuration producing a line-type energy distribution was chosen. The laser fluence was high enough to melt the aluminium and copper layers at the interference maxima but the iron layer remained in the solid state. Thus, diffusive and convective exchange occurred between aluminium and copper at the energy maxima positions leading to periodical alloy formation with a long-range order. Because it remained in solid state, the iron layer at the top acted as a protective layer effectively preventing removal of the molten layers. The interaction of the different layers was characterized using FIB, TEM and EDX in STEM mode.     

Tribochemical investigation of DLC coating in water using stable isotopic tracers

Tribochemical reaction of DLC coating in water was investigated by using a stable isotopic tracer, ¹⁸O labeled water (H₂¹⁸O), to carry out the friction test of DLC coating and 440C ball pair, and using ToF-SIMS to analyze the worn surfaces. The result showed that DLC coating tribochemically reacted with water to form hydrophilic hydroxyl and carboxyl groups on surface, and suggested that the formed hydroxyl mainly combined with the secondary or tertiary carbons on the surface. The surface layer on the counter ball mainly consisted of C from the coating, Cr, Fe from the ball and ¹⁸O from water, and was rich in ¹⁸OH. It is thought that the hydrophilic groups formed at the interfaces play an important role in low friction and wear behaviors of DLC coating and the counter part in a water environment. Comparing with that obtained from the test in D₂O, the result also suggests that hydrogen/deuterium exchange is easy to occur between the products containing OD on the mated ball and some adsorbates in an ambient air environment.