La10(SiO4)6－x(GaO4)xO3－0.5x的合成及其导电性能

以溶胶-凝胶法合成前驱体, 在950 ℃时烧结制得La10(SiO4)6－x(GaO4)xO3－0.5x (x＝0, 0.5, 1.0, 1.5和2.0)陶瓷样品, 通过TG-DTA, XRD, IR和SEM表征, 所得产品为磷灰石相. 以电化学阻抗谱研究了其导电性能, 发现决定电导率大小的因素有两种, 一是间隙氧的数量, 二是晶胞的大小, 两种因素的综合作用, 使得La10(SiO4)5(GaO4)O2.5的电导率最大, 在700 ℃时其电导率达到4.66×10－2 S•cm－1. 离子迁移数和氧分压对电导率的研究表明, 其主要的电荷载体是O2－离子.     

La10-x(SiO4)6O3-1.5x的合成及其导电性能的研究

利用溶胶-凝胶法在800 ℃合成了硅酸盐氧基磷灰石La10-x(SiO4)6O3-1.5x(x=0,0.17,0.33,0.50和0.67),经XRD表征所得产品为磷灰石相.以电化学阻抗谱研究了硅酸盐氧基磷灰石的导电性能,体系的电导率随着间隙氧和阳离子空位数量的增多而加大,La9.33(SiO4)6O2的电导率较La9.5(SiO4)6O2.25大,是由于前者有较多的阳离子空位所致,700 ℃时La10(SiO4)6O3的电导率为7.98×10-3 S·cm-1,比La9.33(SiO4)6O2的电导率提高了5倍.氧分压从105～1 Pa变化时电导率保持不变,证明硅酸盐氧基磷灰石在较宽的氧分压范围内为O2-导电.     

Ga掺杂La9+x/3(GeO4)6-x(GaO4)xO1.5的合成及导电性能研究

利用固相法合成系列Ga掺杂缺陷氧锗氧基磷灰石La9+x/3(GeO4)6-x(GaO4)xO1.5(sx=0,0.5,1,1.5).X射线粉末衍射结果表明:反应物在1350℃烧结24 h即可得到磷灰石结构的纯相产物.700℃时La9.5((GeO4)4.5(GaO4)1.5O1.5的电导率达到3.162×10-3 S·cm-1,是同温度La9(GeO4)6O1.5(1.259×10-3 S·cm-1)电导率的2.5倍.氧分压测试结果表明:材料的电导率在Po2=1～105 Pa保持不变,证明材料在较宽的氧分压范围内为O2-导电.     

Fe2O3掺杂Ce0.8Nd0.2O1.9固体电解质的结构与导电性能

采用溶胶-凝胶法合成SiO2含量小于50×10-6的Ce0.8Nd0.2O1.9(NDC)陶瓷粉体,并将少量Fe2O3加入到NDC体系中,讨论Fe2O3的掺杂对其微观结构及电性能的影响。通过X射线衍射(XRD)等手段对氧化物进行结构表征,交流阻抗谱(AC)测试电性能。研究表明,Fe2O3的掺杂显著提高NDC陶瓷材料的致密度;相比于NDC而言,加入Fe2O3后材料的晶界电导率提高约12倍,总电导率提高约6倍。     

Bi4(Ti1/3Sn2/3)3O12掺杂BaTiO3基X8R陶瓷微观结构与介电性能

研究了Bi4(Ti1/3Sn2/3)3O12掺杂对钛酸钡基陶瓷微观结构和介电性能影响。结果表明,掺杂Bi4(Ti1/3Sn2/3)3O12后钛酸钡基陶瓷晶粒明显长大,同时烧结温度可由1 280℃降低至1 180℃。系统的介电性能和Bi4(Ti1/3Sn2/3)3O12的掺杂量有密切关系。当Bi4(Ti1/3Sn2/3)3O12的掺杂量从0.5mol%增加到2mol%,体系的居里峰被明显压低和展宽,当掺杂量为2mol%时居里峰变得不明显。当Bi4(Ti1/3Sn2/3)3O12的掺杂量从0.5mol%增加到2mol%,系统的居里温度由131℃升高至139℃。当Bi4(Ti1/3Sn2/3)3O12的掺杂量为1mol%时,钛酸钡基陶瓷介电常数为1 930,介电常数温度变化率为5%(-55℃),13%(134℃),-8%(150℃),满足X8R标准。     

La取代Ba对Ba1-xLaxMn3Al9O19-α催化剂结构及甲烷催化燃烧性能的影响

采用以尿素水解为基础的水热合成法制备了La和Mn取代的六铝酸盐催化剂(Ba1-xLaxMn3Al9O19-α).在Mn含量达到阈值时,研究了不同量的La取代Ba对Ba1-xLaxMn3Al9O19-α的相组成、结构、热稳定性及甲烷催化燃烧活性的影响.当x≥0.4时,水热合成过程中生成的La2(CO3)3在530-580℃分解,800-900℃时与-γAl2O3反应生成LaAlO3钙钛矿相,可抑制由BaCO3分解而生成的Ba2+的固相扩散,从而阻止了BaAl2O4尖晶石相的生成,使Ba2+在固相中保持较高的分散性,促进了六铝酸盐(-βAl2O3)相的形成.当x<0.4时,BaAl2O4尖晶石相的存在引起催化剂比表面积和催化燃烧活性的降低.La3+取代Ba2+后,六铝酸盐结构发生一定程度的扭变.这种扭变越大,所形成的六铝酸盐催化剂的热稳定性越差.Ba1-xLaxMn3Al9O19-α催化剂的甲烷催化燃烧活性随x的增大而增加,x=0.8时催化剂的活性最佳.     

Fe2O3与TiF3添加剂对LiBH4-MgH2复合氢化物体系的协同催化作用

通过球磨方法制备出2LiBH4-MgH2,2LiBH4-MgH2-10%Fe2O3,2LiBH4-MgH2-10%TiF3,2LiBH4-MgH2-5%Fe2O3-5%TiF3和2LiBH4-MgH2-10%Fe2O3-10%TiF35个复合氢化物体系,用热重(TG)、差示扫描量热(DSC)、X射线衍射(XRD)、傅里叶变换红外光谱(FTIR)和压力-组成-温度仪(PCT)等对所制备体系进行表征.结果表明,Fe2O3和TiF3的掺杂均能够有效地改善2LiBH4-MgH2复合体系的放氢性能,尤其是两者共掺杂的2LiBH4-MgH2-10%Fe2O3-10%TiF3体系,初始放氢温度为110℃,总放氢量达到约9.6%.对2LiBH4-MgH2-5%Fe2O3-5%TiF3体系的PCT表征结果表明,在400℃时,10 min内放氢量达到了8.6%,放氢热力学和放氢动力学均优于单一相的掺杂,体现了两相掺杂的协同催化作用.     

Sr和Co共掺杂对PrAlO3钙钛矿氧化物的结构和电性能的影响

采用柠檬酸盐法结合高温烧结制备了(Pr,Sr)(Al,Co)O3-δ系列钙钛矿氧化物导电陶瓷。使用X射线衍射(XRD)、扫描电镜(SEM)和直流四线法等手段对样品的物相、微观结构和电性能进行了表征。结果表明:所制备的Pr0.9Sr0.1Al1-yCoyO3-δ(y=0.1~0.5)陶瓷均为单相菱方钙钛矿结构,在掺杂范围内其晶胞体积、相对密度和电导率都随Co掺杂量y的增加而增大,但电导率的增幅在逐步减小;所有陶瓷样品在空气中都是氧离子与电子空穴的混合导体,电导行为符合小极化子跳跃机制。对于Pr1-xSrxAl0.5Co0.5O3-δ(x=0.1~0.4)陶瓷,当x=0.2时样品有较明显的第二相(Pr,Sr)CoO3析出,说明Sr在该体系的固溶限在10~20at%之间,而且随着x的进一步增加,(Pr,Sr)CoO3增多并成为主相;在测量温度范围内,Pr1-xSrxAl0.5Co0.5O3-δ的电导率随x的增加大体呈现出一个先增大后减小的变化趋势,在x=0.3附近达到一个最大值,当x≥0.2时还可观察到明显的半导体-金属性转变,且转变温度随x的增加而逐渐降低。     

SiO44-对Li3Sc2(PO4)3快离子导体的阴离子替代效果研究

Li3Sc2(PO4)3因具有有利的离子传导通道、低的电子电导率和高的稳定性而成为全固态锂离子电池用固体电解质最具竞争力的材料之一,然而这一化合物只有在245℃以上的γ相才具有快离子传导特性。人们主要采用Zr4+、Ti4+等阳离子部分取代其中的Sc3+以改善材料的室温电导率,有关该化合物PO43-阴离子替代的报道还很少。本研究试图利用机械研磨技术,通过向Li3Sc2(PO4)3原料混合物中加入适量SiO2,以期能够实现对该化合物的部分阴离子替代。研究结果表明:所制备的Li3+xSc2(PO4)3-x(SiO4)x(x=0~0.6)系列化合物在x=0.15时电导率达到最大值,σ298=9.55×10-4 S.m-1,离子传导激活能达到最小值45.06 kJ.mol-1。29Si MAS-NMR测试结果证实所加入的SiO2主要以[SiO4]四面体形式存在替代Li3Sc2(PO4)3中部分[PO4]四面体。     

钙掺杂对La2-xCaxCe2O7-δ性能影响研究

利用高温固相反应法制备了高温质子导体La2-xCaxCe2O7-δ(0≤x≤0.2)。分别利用X射线衍射(XRD)、扫描电子显微镜(SEM)对试样的相组成、微观形貌进行了表征。并对试样在水蒸气和CO2气氛中的化学稳定性进行了测试。研究了不同掺杂量和不同测试气氛对La2-xCaxCe2O7-δ电性能的影响。实验结果表明:1 500℃烧结的试样均形成萤石型结构;试样在CO2和水蒸气气氛中表现出良好的化学稳定性。试样在湿润氢气气氛下的电导率明显高于干燥空气气氛,x=0.1的试样在湿润氢气气氛中具有最高的电导率,850℃时达到3.16×10-2S.cm-1,电导活化能为84.93 kJ.mol-1。     

Defect and dopant properties of the Aurivillius phase Bi4Ti3O12

Computer modelling techniques have been used to investigate the defect and oxygen transport properties of the Aurivillius phase Bi₄Ti₃O₁₂. A range of cation dopant substitutions has been considered including the incorporation of trivalent ions (M³⁺=Al, Ga and In). The substitution of In³⁺ onto the Bi site in the [Bi₂O₂] layer is predicted to be the most favourable. The calculations suggest that lanthanide (Ln³⁺) doping at the dilute limit preferentially occurs in the [Bi₂O₂] layer, with probable distribution over both the [Bi₂O₂] and the perovskite A-site at higher dopant levels. It is predicted that the reduction process involving Ti³⁺ and oxygen vacancy formation is energetically favourable. The energetics of oxide vacancy migration between various oxygen sites in the structure have been investigated.     

ALa9(SiO4)6O2.5(A=Ca，Sr，Ba)的合成及其电性能

利用溶胶-凝胶法在850 ℃合成了硅酸盐氧基磷灰石ALa₉(SiO₄)₆O_2.5(A=Ca、Sr和Ba),经XRD表征所得产品为磷灰石相。以电化学阻抗谱研究了ALa₉(SiO₄)₆O_2.5的导电性能,发现A的原子半径越大,体系的电导率越高,活化能却减小。在700 ℃时BaLa₉(SiO₄)     

Li1.3Zr1.7Al0.3(PO4)3的离子交换特性

锂作为21世纪推动科学技术发展的重要元素之一,被誉为“工业味精”、“能源之星”。目前锂及其相关盐类材料已成为信息产业、核能源、航空航天技术、新型材料及军事科技等行业重点开发领域,具有极高科学价值和广阔商业前景[1￣4]。氯化锂是电解制金属锂的主要原料,它的纯度是电     

High temperature crystal structures and superionic properties of SrCl2, SrBr2, BaCl2 and BaBr2

The structural properties of the binary alkaline-earth halides SrCl₂, SrBr₂, BaCl₂ and BaBr₂ have been investigated from ambient temperature up to close to their melting points, using the neutron powder diffraction technique. Fluorite-structured SrCl₂ undergoes a gradual transition to a superionic phase at 900–1100 K, characterised by an increasing concentration of anion Frenkel defects. At a temperature of 920(3) K, the tetragonal phase of SrBr₂ undergoes a first-order transition to a cubic fluorite phase. This high temperature phase shows the presence of extensive disorder within the anion sublattice, which differs from that found in superionic SrCl₂. BaCl₂ and BaBr₂ both adopt the cotunnite crystal structure under ambient conditions. BaCl₂ undergoes a first-order structural transition at 917(5) K to a disordered fluorite-structured phase. The relationship between the (disordered) crystal structures and the ionic conductivity behaviour is discussed and the influence of the size of the mobile anion on the superionic behaviour is explored.     

An experimental investigation of ionic transport properties in CuI-Ag2WO4 and CuI-Ag2CrO4 mixed systems

The phenomenon of ionic transport in the case of two different mixed systems (CuI)_(1−x)-(Ag₂WO₄)_x(0.15?x?0.6) and (CuI)_(1−y)-(Ag₂CrO₄)_y(0.15?y?0.5) has been investigated. Powder X-ray diffraction (XRD) analysis coupled with differential scanning calorimetry (DSC), Fourier transform infrared (FT-IR), FT-Raman and electrical transport studies involving ionic transport number and temperature-dependent electrical conductivity measurements have been carried out in order to identify the various phases responsible for the conduction process. The occurrence of typical ionic conductivity values of 4.5×10⁻³ Scm⁻¹ for the composition (CuI)_0.45-(Ag₂WO₄)_0.55 and 1.1×10⁻⁴ Scm⁻¹ in the case of (CuI)_0.55-(Ag₂CrO₄)_0.45 at room temperature has been discussed in terms of the observed characteristics.     

CaO或BaO与Sm2O3共掺杂CeO2体系电子结构和氧离子迁移的DFT+U研究

使用GGA+U方法研究了CaO或BaO与Sm₂O₃共掺杂CeO₂体系几何和电子结构及氧离子迁移。计算结果表明,Ba和Sm均靠近氧空位时BaSmCe₃₀O₆₃体系最稳定;Sm靠近,Ca远离氧空位时CaSmCe₃₀O₆₃体系最稳定。BaSmCe₃₀O₆₃和CaSmCe₃₀O₆₃体系中均不存在Ce⁴⁺变价。对CaSmCe₃₀O₆₃体系氧离子迁移的研究发现,当氧离子迁移到空位时,迁移能大小顺序为E_m(3→V)< E_m(1→V)< E_m(4→V)< E_m(2→V),这一规律源于氧离子与低价掺杂离子产生负电势之间的排斥作用;对BaSmCe₃₀O₆₃体系氧离子迁移的研究发现,当空位迁移到周围氧离子时,迁移能大小顺序为E_m(V→3)< E_m(V→5)< E_m(V→1),这一规律源于氧空位产生的正电势与低价掺杂离子产生的负电势之间的吸引作用。此外,CaSmCe₃₀O₆₃体系最小迁移能小于SmCe₃₁O₆₃体系,证实了CeO₂-Sm₂O₃-CaO体系离子电导率大于CeO₂-Sm₂O₃体系的实验结果。     

CaO或BaO与Sm2O3共掺杂CeO2体系电子结构和氧离子迁移的DFT+U研究

使用GGA+U方法研究了Ca O或Ba O与Sm2O3共掺杂Ce O2体系几何和电子结构及氧离子迁移。计算结果表明,Ba和Sm均靠近氧空位时Ba Sm Ce30O63体系最稳定;Sm靠近,Ca远离氧空位时Ca Sm Ce30O63体系最稳定。Ba Sm Ce30O63和Ca Sm Ce30O63体系中均不存在Ce4+变价。对Ca Sm Ce30O63体系氧离子迁移的研究发现,当氧离子迁移到空位时,迁移能大小顺序为Em(3→V)Em(1→V)Em(4→V)Em(2→V),这一规律源于氧离子与低价掺杂离子产生负电势之间的排斥作用;对Ba Sm Ce30O63体系氧离子迁移的研究发现,当空位迁移到周围氧离子时,迁移能大小顺序为Em(V→3)Em(V→5)Em(V→1),这一规律源于氧空位产生的正电势与低价掺杂离子产生的负电势之间的吸引作用。此外,Ca Sm Ce30O63体系最小迁移能小于Sm Ce31O63体系,证实了Ce O2-Sm2O3-Ca O体系离子电导率大于Ce O2-Sm2O3体系的实验结果。     

Ionic Mobility, Phase Transitions, and Superionic Conduction in Solid Solutions (100 ? x)PbF2-xZrF4 and Crystals K2ZrF6, (NH4)2ZrF6, KSnZrF7, and M(NH4)6Zr4F23 (M = Li, Na)

Methods of (¹⁹F, ¹H) NMR and impedance spectroscopy are used to investigate the internal mobility and ionic conduction in solid solutions arising in the system PbF₂-ZrF₄ and polycrystals KSnZrF₇, Li(Na)(NH₄)₆Zr₄F₂₃, and M₂ZrF₆ (M = K, NH₄). Factors responsible for the form of ionic motions and their energetics at 170–550 K are considered. It is established that the phase transitions in these compounds are connected with the crystal transition to a superionic state and that the high ionic (superionic) conductivity of beta phases is due to the diffusion of fluoride ions, ammonium cations, and possibly alkali metal cations. The obtained data testify to a substantial role of chainlike aggregation of anionic groupings and a variableness of structural mechanisms of formation of such chains in fluorozirconates for the development of translational diffusion in these compounds.__________Translated from Elektrokhimiya, Vol. 41, No. 5, 2005, pp. 573–582.Original Russian Text Copyright © 2005 by Kavun, Uvarov, Slobodyuk, Goncharuk, Kotenkov, Tkachenko, Gerasimenko, Sergienko.     

LiMg0.5Mn1.5O4的合成及对Li+的离子交换选择性

锂及其化合物在航空航天、化工、医药、空调、高能电池和热核反应等方面都有广泛应用，对锂及其化合物的需求与日俱增。我国液体锂资源非常丰富，开发利用其中的锂资源具有重要意义。从盐湖水、地下卤水、盐田母液、油气田水等咸水资源中提取锂的方法有碳酸盐沉淀法、离子交换法、萃取法等。离子     

Study on the reactivity of In2O3 in mixtures with ammonium-zeolites

In ground mixtures of In₂O₃ and NH₄Y, incorporation of In⁺ cations into the zeolitic phase occurs upon thermal treatment by partial reductive solid-state ion exchange associated with oxidation of ammonium ions or released ammonia to N₂ and NH₂OH. Cationic InO⁺ species, created in zeolites by reductive solid-state ion exchange of In₂O₃/NH₄-zeolite mixtures in hydrogen atmosphere and subsequent oxidation of the In⁺ lattice cations by oxygen, do not undergo autoreduction up to 970 K. Reductive solid-state ion exchange easily proceeds in carbon monoxide atmosphere at temperatures between 620 and 770 K. The significance of these observations for the use of indium-containing zeolites as catalysts is discussed.