多孔La0.6Sr0.4Co0.2Fe0.8O3-δ的制备及表征

多孔Ｌａ０．６Ｓｒ０．４Ｃｏ０．２Ｆｅ０．８Ｏ３－δ陶瓷具有一定的强度、良好的透气和电传导性能,可用于中温ＳＯＦＣ阴极支撑和氧分离膜活性支撑体。本文用固相反应法制备了多孔Ｌａ０．６Ｓｒ０．４Ｃｏ０．２Ｆｅ０．８Ｏ３－δ陶瓷。考察了烧结条件１成型压力有机添加剂量对孔隙率和孔径的影响,研究发现气体渗透随机孔隙率线性增长,电导率随孔隙率的增大而下降,并满足关系式σ＝σ０（１－Ｐ）＾３．１。     

掺杂BaCeO3和SrCeO3在氧,氢及水气气氛下的电导性能

掺杂碱土金属铈酸盐系统：ＭＣｅ１－ｘＲｘＯ３－ｘ／２（Ｍ＝Ｂａ，Ｓｒ；Ｒ＝Ｙｂ，Ｙ，Ｇｄ，Ｌａ；ｘ＝０．０１～０．１０）可由固相反应制得单相化合物，Ｘ射线衍射分析表明，掺杂元素及掺杂量对掺杂ＢａＣｅＯ３和ＳｒＣｅＯ３的晶体结构影响不大。用复数阻抗谱研究了在氧、氢、水气气氛下的电导性能。在各种气氛下ＭＣｅ０．９５Ｙｂ０．０５Ｏ２．９７５（Ｍ＝Ｂａ，Ｓｒ）的电导率最大。根据测试结果，结合缺陷化学理论讨     

Sr1-xBixFeO3-δ(x≤0.50)的柠檬酸盐法制备和导电性

采用柠檬酸法制备了Ｓｒ１－ｘＢｉｘＦｅＯ３－δ（ｘ≤０．５０）系列氧离子－电子混合导体,并采用ＸＲＤ,ＩＲ,ＴＧ,ＤＴＡ和交流复阻抗技术对产物进行了表征。初始凝胶经自燃和８００℃下预烧,可得纯相钙钛矿产物粉体,其结构与ＳｒＦｅＯ３相似,为正交对称性。     

钴掺杂Sr_4Fe_6O_(13)混合导体氧化物结构及透氧测定

用湿化学法合成了Ｓｒ４ＣｏｘＦｅ６－ｘＯ１３±δ系列混合导体氧化物,对其相结构与透氧性能进行了研究．钴离子的引入导致材料中钙钛矿型杂相的出现,Ｘ＝２．０时材料中还产生了ＣｏＯ杂相,ｘ＝２．６时材料呈现钙钛矿型结构．Ｓｒ４Ｆｅ４Ｃｏ２Ｏ１３±δ的相结构还与焙烧温度及环境气氛中的氧浓度密切相关．随着氧浓度的降低,材料从纯相Ｓｒ４Ｆｅ６Ｏ１３结构（纯氧气气氛下）转变为Ｓｒ４Ｆｅ６Ｏ１３结构、钙钛矿型结构和ＣｏＯ共存（空气气氛下）,直至转变为针镍矿结构、 Ｓｒ４Ｆｅ６Ｏ１３结构和 ＣｏＯ共存． Ｓｒ４Ｆｅ６Ｃｏ１３±δ导体膜在ａｉｒ／Ｈｅ氧浓差梯度下的透氧量为 １．５×１０８ｍｏｌ／ｃｍ２·ｓ（８５０℃）,在６５０～８５０℃范围内透氧活化能为７０ｋＪ／ｍｏｌ．     

多孔La_(0.6)Sr_(0.4)Co_(0.2)Fe_(0.8)O_(3-δ)的制备及表征

多孔Ｌａ０．６Ｓｒ０．４Ｃｏ０．２Ｆｅ０．８Ｏ３－δ陶瓷具有一定的强度、良好的透气和电传导性能,可用于中温 ＳＯＦＣ阴极支撑体和氧分离膜活性支撑体．本文用固相反应法制备了多孔Ｌａ０．６Ｓｒ０．４Ｃｏ０．２Ｆｅ０．８Ｏ３－δ陶瓷．考察了烧结条件、成型压力和有机添加剂量对孔隙率和孔径的影响．研究发现气体渗透率随孔隙率线性增长,电导率随孔隙率的增大而下降,并满足关系式σ＝σ０（１— Ｐ）３．１．     

Bi2（Te1—xSex）3单晶生长热力学研究

本工作研究了Ｂｉ－Ｆｅ－Ｓｅ三元相在富Ｂｉ２Ｔｅ３区的相图。测定了Ｂｉ２Ｔｅ３和Ｂｉ２Ｓｅ３从５５０℃到它们的熔点范围内的等浓度线,用移动加热器（ＴＨＭ）法生长Ｂｉ２（Ｔｅ１－ｘＳｅｘ）３（ｘ＝０．０２５和ｘ＝０．０５）。用霍尔（Ｈａｌｌ）效应测定这些化合物在富Ｔｅ区的固线,研究表明,可再生法生长热力学定义的单晶是可能的。     

立方A^4＋M^5＋2O7型化合物与新型负热膨胀材料

概述了立方Ａ＾４＋Ｍ＾５＋２Ｏ７型化合物的结构特点，讨论了ＡＶ２－ｘＰｘＯ７型（Ａ＝Ｚｒ或Ｈｆ；ｘ＝０．１～１．２）及其部分取代的Ａ＾４＋１－ｙＢ＾４＋ｙＶ２－ｘＰｘＯ７型（Ｂ＝Ｔｉ，Ｃｅ，Ｔｈ，Ｕ，Ｍｏ，Ｐｔ，Ｐｂ，Ｓｎ，Ｇｅ或Ｓｉ；ｙ＝０．１～０．４）和Ａ＾４＋１－ｙＣ＾１＋ｙＤ＾３＋ｙＶ２－ｘＰｘＯ７型（Ｃ为碱金属元素，Ｄ为稀土金属元素）材料的负热膨胀性能。     

纳米ZrO2/(1-n)SiO2-nAl2O3介孔复合作的制备与光致发光

采用溶胶－凝胶法和超临界干燥技术制备了（１－ｎ）ＳｉＯ２－ｎＡｌ２Ｏ３（ｎ＝０、０．０１、０．１）混合气凝胶体系，并以此作为载体，成功地将纳米ＺｒＯ２粒子组装到（１－ｎ）ＳｉＯ２－ｎＡｌ２Ｏ３介孔体系中，而形成纳米ＺｒＯ２／（１－ｎ）ＳｉＯ２－ｎＡｌ２Ｏ３介孔复合材料。光致发光光谱研究表明，室温下以３１６ｎｍ（３．９２ｅＶ）波长激发时，纳米ＺｒＯ２粒子５４０ｎｍ（２．３０ｅＶ）荧光峰，在介孔复合体     

八种新功能晶体的比热及其与相变掺杂物关系的实验研究

本文对八种新型功能晶体Ｌｉ２Ｂ４Ｏ７、Ｂｉ１２ＴｉＯ２０、Ｂｉ１２ＧｅＯ２０、Ｂｉ１２ＧｅＯ２０、Ｂｉ４Ｇｅ３Ｏ１２、Ｓｒ１－ｘＢａｘＮｂ２Ｏ６（ｘ＝０．３３，０．４８）、ＬｉＴａＯ３等在１３０～９７３Ｋ范围内的比热行为及其与相变、组分之间的关系进行了实验研究，给出了比热的多项式拟合方程，并与用纽曼－卡普定律及用Ｗｉｋｅｌｍａｎｎ经验方程的比热计算值作了对比，为晶体比热的估算提供了依据和方法。     

Ni42Cr6Fe封接合金氧化膜和氧化物晶须的结构

用ＴＥＭ、Ｘ－Ｒａｙ、ＳＥＭ等技术研究了Ｎｉ４２Ｃｒ６Ｆｅ玻封合金在高温湿Ｈ２中形成的氧化膜及氧化物晶须的结构。结果表明：氧化膜主要由Ｃｒ２Ｏ３和（Ｆｅ，Ｍｎ）Ｃｒ２Ｏ４两组相成，氧化膜底层是以Ｃｒ２Ｏ３为主的组织，氧化膜表层是以（Ｆｅ，Ｍｎ）Ｃｒ２Ｏ４为主的组织；Ｓｉ在氧化膜与合金界面分布，Ａｌ则在内氧化层中形成内氧化物质点；氧化膜表面生长的氧化物晶须的杆部为（Ｆｅ，Ｍｎ）Ｃｒ２Ｏ４单晶，头部为     

Cr掺杂Ba0.5Sr0.5Co0.8Fe0.1Cr0.1O3-δ钙钛矿型膜的透氧性能研究

采用固相反应法合成了钙钛矿型Ba0.5Sr0.5Co0.8Fe0.2-xCrxO3-δ(x=0.00,0.10)透氧膜粉体。利用XRD和SEM研究了Ba0.5Sr0.5Co0.8Fe0.2-xCrxO3-δ(x=0.00,0.10)的晶体结构和烧结性能,考察了在700~850℃范围内Ba0.5Sr0.5Co0.8Fe0.2-xCrxO3-δ(x=0.00,0.10)膜片的氧渗透性能。结果表明,它们均显示出优良的透氧性能,850℃时的透氧量分别为1.05mL/(min.cm2)、0.85mL/(min.cm2)。透氧稳定性的研究表明,Cr掺杂Ba0.5Sr0.5-Co0.8Fe0.1Cr0.1O3-δ在800℃时显示出较高的稳定性,证实用Cr离子部分取代Ba0.5Sr0.5Co0.8Fe0.2O3-δ的Fe离子能明显提高钙钛矿的结构稳定性。     

Structural,Sintering and Electrical Properties of Cr-doped La0.6Sr0.4CrxFe1-xO3-δ（x=0.10,0.20） Oxides

The perovskite Cr-doped La0.6Sr0.4CrxFe1-xO3-δ(x=0.10,0.20) oxides were synthesized via the citrate gel method.The perovskite forming of the La0.6Sr0.4CrxFe1-xO3-δ(x=0.10,0.20) oxides were studied by thermogravimetric analysis(TG),differential scanning calorimetry(DSC),and X-ray diffraction(XRD).Structural and chemical stability under H 2-containing helium atmospheres of La0.6Sr0.4CrxFe1-xO3-δ(x=0.10,0.20) were investigated by TG and XRD.The sintering microstructures of the perovskite La0.6Sr0.4CrxFe1-xO3-δ(x=0.10,0.20) ceramics were investigated by scanning electron microscopy(SEM),and the electrical conductivities of both oxide ceramics were also measured up to 900 C.The results demonstrated that the chemical stability of the Co-free La0.6Sr0.4CrxFe1-xO3-δ(x=0.10,0.20) oxides was significantly improved compared to the Co-containing La0.6Sr0.4Co0.2Fe0.8O3-δ and Ba0.5Sr0.5Co0.8Fe0.2O3-δ oxides.The incorporation of Cr cations in the B-site of the pervoskite oxides resulted in the improved structural and chemical stability of the as-synthesized La0.6Sr0.4CrxFe1-xO3-δ(x=0.10,0.20) oxides.     

Sr、Co共掺多铁性材料BiFeO3的性能

利用溶胶-凝胶法制备了BiFeO_3、Bi_(0.95)Sr_(0.05)FeO_3、BiFe_(0.95)Co_(0.05)O_3和Bi_(0.95)Sr_(0.05)Fe_(0.95)Co_(0.05)O_3样品,并对样品的结构、形态、元素含量、铁电性和铁磁性进行了研究。结果表明,共掺杂样品Bi_(0.95)Sr_(0.05)Fe_(0.95)Co_(0.05)O_3的晶体结构发生了变化,铁电性明显增强,但漏电流变大;Bi_(0.95)Sr_(0.05)FeO_3、BiFe_(0.95)Co_(0.05)O_3样品的磁性都有所增强,但Bi_(0.95)Sr_(0.05)Fe_(0.95)Co_(0.05)O_3样品的磁性并没有随着Sr和Co的共同掺杂而进一步提高,从氧空位浓度、Fe-O共价键结构的变化和晶体尺寸三个方面对产生这种现象的原因进行了分析。     

Sr~(2+)掺杂及非化学计量LaFeO_3的溶剂热制备及光催化性能

利用简单的溶剂热法制备LaFeO_3、La_(0.8)Sr_(0.2)FeO_(3-δ)以及非化学计量的La_(0.8)Sr_(0.2)FeO_(3-δ)(x=0.97,1.03)纳米颗粒。采用XRD、TEM、UV-Vis、XPS等手段对样品的形貌和结构进行表征,以孔雀石绿(MG)光降解为模型反应,在最大吸收波长下(616.9nm)考察材料的光催化性能。结果表明:Sr~(2+)的掺入减小了晶粒尺寸,致使晶体产生晶格畸变并形成氧空位V··O,抑制电子-空穴重组,增大量子效率;掺入Sr~(2+)并改变非化学计量,使得催化剂在可见光区域有较强的光吸收,比表面积增大,其中(La_(0.8)Sr_(0.2))1.03FeO_(3-δ)的比表面积最大(20.164 4m2/g),可见光降解效率也最高(83.8%)。Sr~(2+)掺杂及非化学计量LaFeO_3的可见光催化活性均高于纯LaFeO_3。     

La0.67Sr0.33MnO3中Bi的掺杂效应

将Bi2O3掺杂到用溶胶—凝胶法制备的La0.6Sr0．33MnO3(LSMO)微粉中,XRD测量结果证实有过量的Bi析出。随着Bi掺杂量的增加,LSMO／(Bi2O3)x/2材料电阻率发生明显变化,在x=(0—0．10)摩尔比的掺杂范围内,电阻率先上升后突然下降。当X=0．1时,电阻率比未掺杂样品下降了一个数量级。Bi掺杂对低温和室温磁电阻有着完全不同的影响。低温下,随掺杂量增加,磁电阻下降;室温下Bi的微量掺杂可以使磁电阻增大,掺入x=0.03Bi使室温磁电阻由-4.4％提高到-5．6％。     

Photocatalytic performance of nanocrystalline Bi5Ti3FeO15 layered perovskite under visible light

Nanocrystalline Bi5Ti3FeO15 layered perovskite exhibiting Aurivillius phase was synthesized by polymerized complex (PC) method and investigated for its physico-chemical as well as optical properties. The crystallization of Bi5Ti3FeO15 synthesized by PC method was found to occur in the temperature range of 800-1050 degress C, whereas the single crystalline Bi5Ti3FeO15 formed at 1030 degrees C by solid state reaction (SSR) method. The observation of highly pure phase and such lower crystallization temperature in Bi5Ti3FeO15 prepared by PC method, is in total contrast to that observed in Bi5Ti3FeO15 prepared by the conventional solid-state reaction (SSR) method. The band gap of nanocrystalline Bi5Ti3FeO15 determined from UV-Vis diffusion reflectance spectrometer was 2.38 eV (525 nm). The photocatalytic activity of Pt/Bi5Ti3FeO15 prepared by PC method was investigated with the photodecomposition of isopropyl alcohol (IPA) and hydrogen production from water-methanol mixed solution under visible light (lambda > or = 420 nm). The respective activities for PC sample were higher than that of Pt/Bi5Ti3FeO15 prepared by SSR as well as Pt/TiO(2-x)N(x).     

多铁性xBi_(0.9)Dy_(0.1)FeO_3-(1-x)CoFe_2O_4复合粉体的制备与表征

采用柠檬酸盐自燃烧法制备Bi0.9Dy0.1FeO3粉体,溶液法合成xBi0.9Dy0.1FeO3-(1-x)CoFe2O4复合粉体,得到了同时具有铁电性能和铁磁性能的铁酸铋基多铁性材料。研究了粉体的微观结构、铁电性能和铁磁性能。结果表明:当x从0.9减少到0.4,在最佳煅烧温度合成的Bi0.9Dy0.1FeO3-CoFe2O4复合粉体的磁极化强度和剩余极化强度都随着x先增大后减少。Bi0.9Dy0.1FeO3与CoFe2O4复合使铁电性能和铁磁性能均有所提高,当x=0.5时,在700℃的煅烧温度下,获得较好的铁电和铁磁性能,其中Vc=3 268.241Oe,Ms=37.05emμ/g。     

锶镁共掺对Na0.5Bi0.5TiO3氧离子导体电学性能的影响分析

通过固相反应法制备单一结构的锶镁共掺的Na0.5Bi0.48Sr0.02Ti0.98Mg0.02O2.97氧离子导体,利用交流阻抗谱和内耗温度谱分别研究锶镁共掺对Na0.5Bi0.5TiO3材料晶粒电导率及氧离子扩散的影响。在593K时,Na0.5Bi0.48Sr0.02Ti0.98Mg0.02O2.97材料的晶粒电导率可以达到5.31×10^-4S/cm,比母体Na0.5Bi0.5TiO3材料在同温度下的晶粒电导率高一个数量级,甚至超过了Na0.5Bi0.5Ti0.98Mg0.02O2.98样品在673K温度下的晶粒电导率。在锶镁共掺的Na0.5Bi0.48Sr0.02Ti0.98Mg0.02O2.97材料中观察到一个氧弛豫内耗峰,其弛豫参数为:E=0.85eV,τ0=7.4×10^-14s。结合弛豫参数和结构分析,Sr^2+的掺杂在一定程度上可以增大氧离子扩散的自由体积,较大的自由体积、较高的可动氧空位浓度和较好的氧空位可动性是NBT-SrMg2样品晶粒电导率相较于NBT-Mg2样品大幅提高的主要原因。     

Effects of La concentration on the structural and dielectric properties of 0.57BiFeO3-0.43PbTiO3 crystalline solutions

Crystalline solutions of 0.57(Bi(1-x)La(x))FeO(3)-0.43PbTiO(3) (BLF-PT) for x = 0, 0.1, 0.2, and 0.3 were fabricated by the traditional solid state reaction method. X-ray diffraction analysis revealed that the tetragonal torhombohedral phase transformation of BLF-PT occurred with an increase of the La content. The dielectric and ferroelectric properties of BLF-PT were investigated at room temperature for different La contents. BLF-PT revealed strong ferroelectric characteristics for the lower La composition, and transferred to relaxor ferroelectrics for x 0.2. The dielectric constant and remanent polarization were 1461 and 33.5 microC/cm(2), respectively, for BLF-PT of x = 0.2. The dielectric constant and polarization of BLF-PT were enhanced simultaneously with increasing La content. Our results demonstrate that BLF-PT is a competitive piezoelectric ceramic.