(Zn，M)TiO3(M=Co，Ni，Co0.5Ni0.5)固溶体的溶胶-凝胶法合成

通过改进的溶胶-凝胶工艺在低温(800 ℃)下合成了基于钛酸锌(ZnTiO₃)体系的(Zn_1-xCo_x)TiO₃、(Zn_1-xNi_x)TiO₃和[Zn_1-x(Co_0.5Ni_0.5)_x]TiO₃陶瓷固溶体。采用X射线衍射分析(XRD)和差示扫描量热法(DSC)等测量技术对产物进行了物相和热稳定性分析。XRD结果表明，获得单一六方相(Zn_1-xCo_x)TiO₃、(Zn_1-xNi_x)TiO₃和[Zn_1-x(Co_0.5Ni_0.5)_x]TiO₃时各自的固溶稳定区间为0.5 ≤ x ≤ 1.0, 0.9 ≤ x ≤ 1.0和0.8 ≤ x ≤ 1.0。与此同时，热分析结果证实，伴随钛酸锌基陶瓷体系掺杂钴量的增加，其六方相的热稳定性提高，且效果比掺杂镍更加显著。     

Ba0.98Bi0.02(Ti0.9Zr0.1)1-xCuxO3陶瓷的介电性能、弛豫行为与结晶化学特性

采用固相合成法, Bi3+作施主掺杂A位, Cu₂₊作受主掺杂B位, 制备了Ba_0.98Bi_0.02(Ti_0.9Zr_0.1)_1-xCu_xO₃(x=0, 0.01, 0.02, 0.03)陶瓷样品。借助XRD、LCR等研究了该陶瓷的结构与介电性能。结果表明:当x=0.03时, 陶瓷样品出现第二相。通过GULP模拟, 缺陷偶极子的稳定性从低到高依次为:[2Bi_Ba^·+V_Ba"]、[2Bi_Ba^·+Cu_Ti/Zr"]、[Cu_Ti/Zr"+V_O^··], 结合实验可知:介电弛豫程度与晶体中缺陷偶极子的存在形式相关, 其中x=0.01时, 晶体中以[2Bi_Ba^·+Cu_Ti/Zr"]为主。随Cu₂₊掺杂量的增加, 介电常数增加, 介电常数与B位键价和呈反比变化、与八面体BO₆的体积呈正比变化。     

La2(Mo1-xVx)2O9-α的制备及其导电性

采用固相法合成了系列陶瓷样品La₂(Mo_1-xV_x)₂O_9-α (x=0.02, 0.04, 0.06, 0.08). 粉末X射线衍射(XRD)结果表明样品具有单一立方相La₂Mo₂O₉结构. 采用气体浓差电池、电化学阻抗等电化学方法研究了陶瓷样品在823-1123 K下的导电特性. 系列陶瓷样品已完全抑制La₂Mo₂O₉母体在853 K附近的相变; 各样品在干燥及湿润氧气气氛中几乎为纯氧离子导体, 质子导电性可忽略不计; 氧离子电导率σ随掺杂离子浓度的变化为σ(x=0.02)<σ(x=0.08)<σ(x=0.06)<σ(x=0.04), 这与晶胞自由体积大小的次序完全一致, x=0.04样品具有最高的氧离子电导率0.051 S·cm^-1; 氧分压与电导率的关系表明, 在高氧分压气氛中样品是纯的氧离子导体, 在低氧分压气氛中是氧离子与电子的混合导体.     

锶掺杂对La1-xSrxNbO4-σ质子导体性能的影响

利用高温固相反应法制备了Sr掺杂LaNbO₄质子导体La_1-xSr_xNbO_4-σ(0≤x≤0.02),并且对其性能进行了表征。XRD分析表明,所有的样品具有单斜结构,晶胞体积随Sr掺杂量的增加而增大;La_1-xSr_xNbO_4-σ样品在沸水中和二氧化碳气氛中具有很好的化学稳定性。SEM分析表明,La_1-xSr_xNbO_4-σ粉体经1500℃烧结8h后均得到致密的、晶粒均匀的样品;Sr的掺杂抑制了陶瓷体裂缝的产生和晶粒的过度增长;随Sr的掺杂量增加,晶粒变小。交流阻抗谱分析表明,Sr掺杂改变了LaNbO₄的电导率,其中样品La_0.995Sr_0.005NbO_4-σ具有最高的电导率;样品在25℃水汽饱和的5%H₂-Ar气氛下的电导率明显高于干燥空气气氛,在800℃时,La_0.995Sr_0.005NbO_4-σ电导率达到0.003S·cm^-1,电导活化能为0.44eV。     

Li[Ni1/3Mn1/3Co1/3]O2掺杂Mo研究

采用高温固相合成法制备了Li[Ni_(1－x)/3Mn_(1－x)/3Co_(1－x)/3Mo_x]O₂ (x＝0, 0.005, 0.01, 0.02). 对它们进行了XRD, SEM, 循环伏安及充放电容量测试, 结果发现, 掺杂x＝0.01 Mo的样品具有较高的嵌锂容量和良好的循环稳定性, 在20 mA/g放电电流密度和2.3～4.6 V的电压范围内具有211.6 mAh/g的首次放电比容量, 循环50周后放电比容量仍能达到185.9 mAh/g, 容量损失为12.1%.     

Mn1-x(Li,Ti)xCo2O4尖晶石型复合氧化物的制备、表征与催化性能

用柠檬酸配位燃烧法合成了Mn_1-x(Li,Ti)_xCo₂O₄系列尖晶石型复合氧化物催化剂，使用FTIR和XRD方法对催化剂结构进行表征，通过程序升温氧化反应(TPO)技术对这些催化剂在模拟柴油机尾气条件下进行同时消除NO_x和柴油碳黑反应的活性评价。结果表明，掺杂Li或Ti后的Mn_1-x(Li,Ti)_xCo₂O₄系列催化剂仍然保持了完整的尖晶石型复合氧化物结构，这些催化剂对同时消除柴油机尾气中的碳黑颗粒和NO_x具有良好的催化性能，其中Li或Ti的掺杂量为x=0.05较佳，结合碳黑燃烧与NO_x还原总的催化效果，Mn_0.95Li_0.05Co₂O₄具有最好的催化活性。     

Li[Ni1/3Mn1/3Co1/3]O2掺杂Mo研究

采用高温固相合成法制备了Li[Ni_(1－x)/3Mn_(1－x)/3Co_(1－x)/3Mo_x]O₂ (x＝0, 0.005, 0.01, 0.02). 对它们进行了XRD, SEM, 循环伏安及充放电容量测试, 结果发现, 掺杂x＝0.01 Mo的样品具有较高的嵌锂容量和良好的循环稳定性, 在20 mA/g放电电流密度和2.3～4.6 V的电压范围内具有211.6 mAh/g的首次放电比容量, 循环50周后放电比容量仍能达到185.9 mAh/g, 容量损失为12.1%.     

BaCe0.8-xNbxGd0.2O3-δ(0≤x≤0.45)的制备及性能研究

采用高温固相反应法制备了质子导体BaCe_0.8-xNb_xGd_0.2O_3-δ(0≤x≤0.45)。结合XRD、SEM、EIS等技术对其物相、微观形貌、稳定性及电导率进行了研究。结果表明,在1 600 ℃烧结5 h制备的质子导体BaCe_0.8-xNb_xGd_0.2O_3-δ(0≤x≤0.45)均能保持主相为斜方晶的钙钛矿结构。Nb的加入可明显提高烧结样品的致密性及在CO₂和水蒸气气氛下的稳定性。在湿润H₂/Ar(0.4%,V/V)气氛中800 ℃下,x=0.1样品的电导率为5.73 mS·cm^-1,电导活化能为0.35 eV,与x=0的样品相当。     

NbS2-xSex的制备、表征及其摩擦学性能

本文采用固相反应合成了NbS_2-xSe_x纳米材料。并分别采用XRD、SEM、TEM、HRTEM进行了结构、形貌和成分的分析表征。系统研究了合成温度、保温时间及不同掺杂量对产物晶型和形貌演化的影响及规律性。结果表明Se的掺杂使NbS_2-xSe_x的形貌由纳米带(板)转变为纳米片,衍射峰明显宽化,峰强变弱,晶粒细化。且掺杂量、保温温度及时间对产物的形貌影响较大;在750℃下保温2h得到的掺杂5at%Se的NbS_1.9Se_0.1形貌良好。将NbS_2-xSe_x作为液体石蜡油的添加剂的UMT-2摩擦学实验结果表明掺杂后的NbS_2-xSe_x具有优异的摩擦性能,其中掺杂5at%的Se在750℃下保温2h的NbS_1.9Se_0.1摩擦性能最佳,同时对其摩擦机理进行了解释。     

固体电解质La2-xCaxMo1.7W0.3O9-δ(0≤x≤0.2)的合成、表征及电性能

在氧离子导体La₂Mo_1.7W_0.3O₉的基础上，采用固相法合成了La位掺杂的Ca系列新型氧化物La_2-xCa_xMo_1.7W_0.3O_9-δ(0≤x≤0.2)。通过XRD、Raman和XPS等手段对化合物结构进行表征，交流阻抗谱测试其电性能。结果表明：掺杂离子Ca²⁺的半径小于基质离子La³⁺的半径导致晶格收缩；Ca的掺杂在La₂Mo_1.7W_0.3O₉自身内置氧空位的基础上增加了额外的氧空位，提高了氧离子导体的电导率，550 ℃电导率由0.79 × 10^-4 S·cm^-1 (x=0.0)增加到1.5 × 10^-4 S·cm^-1 (x=0.16，0.2)，电导率增加89.9%。     

Preparation and hydrogen permeation of SrCe0.95Y0.05O3−δ asymmetrical membranes

Asymmetrical thin membranes of SrCe_0.95Y_0.05O_3−δ (SCY) were prepared by a conventional and cost-effective dry pressing method. The substrate consisted of SCY, NiO and soluble starch (SS), and the top layer was the SCY. NiO was used as a pore former and soluble starch was used to control the shrinkage of the substrate to match that of the top layer. Crack-free asymmetrical thin membranes with thicknesses of about 50 μm and grain sizes of 5–10 μm were successfully pressed on to the substrates. Hydrogen permeation fluxes (J_H2) of these thin membranes were measured under different operating conditions. At 950 °C, J_H2 of the 50 μm SCY asymmetrical membrane towards a mixture of 80% H₂/He was as high as 7.6 × 10⁻⁸ mol/cm² s, which was about 7 times higher than that of the symmetrical membranes with a thickness of about 620 μm. The hydrogen permeation properties of SCY asymmetrical membranes were investigated and activation energies for hydrogen permeation fluxes were calculated. The slope of the relationship between the hydrogen permeation fluxes and the thickness of the membranes was −0.72, indicating that permeation in SCY asymmetric membranes was controlled by both bulk diffusion and surface reaction in the range investigated.     

Pt/SrZr0.95Y0.05O3-TiO2-xNx复合催化剂的制备及模拟太阳光催化产氢活性研究

利用共沉淀法和固相法制备出SrZr_0.95Y_0.05O₃微粒,采用溶胶包覆法使其与含氮TiO₂溶胶复合,并原位光沉积Pt颗粒组装成异质结复合催化剂,采用XRD、TG-DTA、紫外可见漫反射光谱(UV-Vis DRS)和荧光光谱(FS)等技术对其进行了表征和分析,以草酸为牺牲剂,模拟太阳光下光催化产氢为探针,评价了催化剂的光催化活性。研究了不同氮源剂、烧结温度、载铂含量对催化剂光催化产氢活性的影响。结果表明,在模拟太阳光照射下,单独的SrZr_0.95Y_0.05O₃和TiO₂几乎不产生氢气;而将两者采用溶胶包覆法复合并掺氮后,所制备出的复合催化剂表现出一定程度的产氢活性,在氮源剂为三乙胺、400 ℃焙烧下具有最佳的产氢活性,催化活性的提高源于复合催化剂中形成的异质结抑制了光生载流子的快速复合以及氮掺杂引起对可见光的响应;进一步负载铂后,其产氢量得到大幅度的提高,其最佳负载量为1wt%,6 h内产氢量达到12.5 mmol,是未负载的样品的22倍多,这是由于铂负载进一步抑制了光生载流子的复合,从而大大地提高了光催化活性。     

Electrochemical properties and synthesis of LiAl0.05Mn1.95O3.95F0.05 by a solution-based gel method for lithium secondary battery

The cathode materials, LiMn₂O₄, LiAl_0.05Mn_1.95O₄ and LiAl_0.05Mn_1.95O_3.95F_0.05 were firstly prepared by a simple solution-based gel method using the mixture of acetate and ethanol as the chelating agent. The synthesized samples were investigated by X-ray diffraction, scanning electronic microscope and differential and thermal analysis. The as-prepared powders were used as positive materials for lithium-ion battery, whose discharge capacity and cycle voltammogram properties were examined. The results revealed that LiAl_0.05Mn_1.95O_3.95F_0.05 synthesized by the solution-based gel method had higher initial capacity than LiAl_0.05Mn_1.95O₄ and better capacity retention rate (92%) than that of LiAl_0.05Mn_1.95O₄ and LiMn₂O₄, which revealed that Al and F dual-doped LiMn₂O₄ could gain better electrochemical properties of LiMn₂O₄ than only the Al-doped LiMn₂O₄.     

Ba0.95Ce0.90Y0.10O3-α固体电解质的质子导电性

本文通过高温固相反应合成了Ba_0.95Ce_0.90Y_0.10O_3-α固体电解质,测定了该固体电解质高温(600～1000℃)下的氢的电化学透过(氢气泵)速度。结果表明,该固体电解质在本实验条件下具有良好的质子导电性,其质子迁移数为0.8～1,在600～700℃的较低温度下,几乎显示纯粹的质子导电性。     

LiNi0.8Co0.15Al0.05O2正极材料的FePO4包覆改性

使用液相包覆工艺对LiNi_(0.8)Co_(0.15)Al_(0.05)O_2(NCA)材料进行FePO_4包覆改性,利用FePO_4优异的结构稳定性与热稳定性,对NCA的长期可靠性与安全性能进行改良。重点研究FePO_4包覆对NCA材料的改性效果,以及不同包覆量造成的NCA材料电化学性能差异。表面包覆的FePO_4保护层,能够防止NCA材料与电解液直接接触发生副反应,抑制长期循环过程中过渡金属离子的溶出,保持结构的长期稳定性。当包覆量为1.0%(w/w)时,NCA材料表现出最优的综合性能,充放电循环800次后,容量保持率依然高达95%,25℃下存储100 d后,容量保持率也高于95%,达到了兼顾能量密度、使用寿命及安全性能的理想效果。     

Ni0.8Co0.15Al0.05C2O4@Graphene的合成及电化学性能研究

过渡金属氧化物/石墨烯复合材料具有优异的电化学性能被广泛应用在锂离子电池中。本文以硫酸镍、硫酸钴、硫酸铝、草酸为原料按一定的物质的量比配制成溶液,在120°C的条件下水热反应12小时,得到多元过渡金属氧化物前驱体Ni_0.8Co_0.15Al_0.05C₂O₄(NCA-C₂O₄);该前驱体经聚烯丙基胺盐酸盐修饰后,与氧化石墨烯进行复合并还原得到石墨烯包覆的多元过渡金属氧化物/石墨烯负极材料Ni_0.8Co_0.15Al_0.05C₂O₄@Graphene(NCA-C₂O₄@G)。对材料的结构、形貌和电化学性质进行了表征。扫描电镜测试结果显示样品粒度均一,具有两端不规则长方体形貌。电化学性能测试结果表明：石墨烯包覆后的NCA-C₂O₄@G充放电容量高于前驱体NCA-C₂O₄,NCA-C₂O₄@G复合材料在0.1C电流密度 (1C=1000 mAh/g)下首次放电比容量为1956 mA h/g;经过0.1C、0.2C、0.5C、1C、2C高倍率循环后,当测试电流密度恢复至100 mA/g时,复合材料比容量可迅速回升至720 mA h/g,并在随后50次循环中比容量保持稳定,显示出良好的循环稳定性和倍率性能。     

富锂掺杂Li1.06Co0.05Cr0.1Mn1.85O4的合成及电化学性能研究

锂离子电池具有比能量高、功率大、使用寿命长、无记忆效应、性能价格比高等优点,从而成为可充式电源的主要选择对象.锰由于资源丰富、价廉、环境友好等优点,使锰酸锂(LiMn2O4)成为最有希望取代钴酸锂的正极材料.但锰酸锂的放电容量相对较低,结构欠稳定,容量衰减严重,作为正极材料还无法与钴酸锂相比,近年来做了大量的研究工作以改善它的电化学性能[1～6].最近Youngjoon Shin等研究发现[7]用少量的Li与Ni共同替代LiMn2O4中的Mn得到的LiMn2-2yLiyNiyO4的电化学性能要优于单元素替代的LiMn2-xMxO4(M=Li,Cr,Fe,Co,Ni)的电化学性能.     

Preparation, characterization and the standard enthalpy of formation of La0.95MnO3+δ and Sm0.95MnO3+δ

Among the perovskites, the rare earth manganites find application in several electrochemical devices because of their enhanced thermodynamic stability. In this paper, we present the results obtained on the preparation and characterization of La_0.95MnO_3+δ and Sm_0.95MnO_3+δ which were prepared by the solid state and sol–gel methods. XRD characterization of the manganites indicated that the crystal structure depends on the method of preparation and heat treatments. The ratio of Mn³⁺ to Mn⁴⁺ in these samples also depended on the method of preparation and heat treatments, as indicated by thermogravimetric (TG) and temperature programmed reduction (TPR) studies in Ar + 5% H₂ atmosphere. The standard molar enthalpy of formation, which is a measure of the thermodynamic stability of these compounds were determined using an isoperibol calorimeter.     

LiNi0.8Co0.15Al0.05O2制备过程中聚乙烯吡咯烷酮的加入对其电化学性能的影响

为提高LiNi_(0.8)Co_(0.15)Al_(0.05)O_2(NCA)材料的电化学性能,在NCA材料的制备过程中加入聚乙烯吡咯烷酮(PVP),通过调控所得NCA材料的形貌来提高其电化学性能。所得材料采用X射线衍射仪和扫描电子显微镜进行形貌结构表征,电化学性能经组装成纽扣电池,用电池程控测试仪和电化学工作站进行测试。研究结果表明:由于PVP的空间效应和静电作用,PVP改性的NCA材料拥有更完整的棒状结构、发育出更好的层状结构,电化学储能性能得到较大的提升。在0.1C下,材料的首次放电比容量和充放电效率分别从143.36 mAh·g~(-1)、78.25%提高到了170.24 mAh·g~(-1)、89.20%;在0.2C的实验室条件下循环50次后,容量保持率为94.28%。     

Preparation of LaFe0.95Pd0.05O3 perovskites and their catalytic performances in methane combustion

The physic-chemical properties of LaFe0.95Pd0.05O3 perovskites were strongly dependent on the temperature of calcination. Most of the organic substances and inorganic impurities were readily removed at 723 K but single-phase and well crystallized perovskite structure was formed at 873 K. With further raising the calcination temperature, the crystallite size of LaFe0.95Pd0.05O3 increased considerably. The LaFe0.95Pd0.05O3 sample that calcined at 1073 K showed only comparable activity as the reference LaFeO3 catalyst, in particular below 923 K, but pre-treatment with the reaction gas at 1223 K resulted in significantly enhanced activity due to the generation of active PdO species on the surface. The hysteresis feature upon heating-cooling cycle further confirmed the strong interaction between Pd and LaFeO3 in the perovskite structure.