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.     

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.     

Ca2-3xLa8+2x□x(SiO4)6O2的合成及其导电性能的研究

The silicate oxyapatites Ca_2-3xLa_8+2x□_x(SiO₄)₆O₂(x=0, 0.17, 0.33, 0.50, 0.67) was synthesized via a sol-gel method at low temperature. The apatite phases have been characterised by X-ray diffraction (XRD), conducting properties was studied by electrical chemistry impedance spectroscopy (EIS). The conductivity of La_9.33□_0.67(SiO₄)₆O₂ is 1.58×10^-3 S·cm^-1 at 700 ℃, it is higher about 4 270 times than that of Ca₂La₈(SiO₄)₆O₂, the activation energy is decreasing from 1.37 eV to 0.84 eV. With cation vacancies increasing,the conducting mechanism is gradually translation from a direct linear pathway free oxygen ion conduction to a curve pathway interstitial oxygen ion conduction. The electrical conductivities is almost independent of the oxygen partial pressure, this suggests that the oxyapatites exhibited almost pure O^2- ion conduction over a wide range of oxygen partial pressure.     

Ca2Y8（SiO4）6O2：RE（RE=Eu,Tb）发光薄膜的制备及发光性能的研究

采用溶胶－凝胶法制备了稀土离子掺杂（Eu^3 ,Tb^3 )的氧磷灰石三元稀土硅酸盐Ca2Y8(SiO4)6O2发光薄膜。通过X射线衍射（XRD）,红外光谱（IR）,扫描电镜（SEM）等方法对薄膜的组成、结构、颗粒尺寸、形貌及厚度进行了研究,通过发光光谱对薄膜的发光性质进行了分析。XRD结果表明700℃时薄膜尚处于非晶态,800℃时已开始有Ca2Y8(SiO4)6O2的物相形成,1000℃时结晶已完全。这一点和红外光谱的结果相符。发光光谱测试表明Ca2Y8(SiO4)6O2:Eu^3 薄膜显示了很强的红光发射,并以Eu^3＋的^5D0-^7F2(616nm)超灵敏跃迁为最强一组。Ca2Y8(SiO4)6O2:Tb^3 的发射光谱由蓝光发射和绿光发射两部分组成,前者对应于^5D3-^7FJ,后者对应于^5D4-^7FJ(J=6,5,4,3),且以^5D4-^7F5(544nm)绿光发射为最强。     

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+xMn2O4的溶胶-凝胶法合成及其电化学性能

锂离子电池;锂锰氧化物;尖晶石结构;Li1+xMn2O4的溶胶-凝胶法合成及其电化学性能     

CuO/Ce0.5Ti0.5O2的制备与表征及其对NO+CO反应的催化活性

以Ce0.5Ti0.5O2为载体, 采用浸渍法制备了不同负载量的CuO/Ce0.5Ti0.5O2催化剂, 通过TPR、XRD和激光Raman光谱等技术对其进行了表征, 并在色谱-微反装置上考察了催化剂对NO+CO反应催化性能. 结果表明, CuO/Ce0.5Ti0.5O2催化剂对NO+CO反应的活性与CuO负载量有关; 500 ℃焙烧的催化剂, 当CuO的负载量(w)为22%时, 催化剂的活性最好; 14%CuO/Ce0.5Ti0.5O2在700 ℃焙烧具有最佳催化活性, 这可能与复合载体形成了CeTi2O6的结构有关. TPR结果表明, CuO在Ce0.5Ti0.5O2上出现了四种还原能力不同的物种, α和β峰是载体表面高度分散的CuO物种, γ峰是与Ce0.5Ti0.5O2相互作用较强的孤立CuO晶簇的还原峰, δ峰是载体表面晶相CuO的还原峰; XRD结果表明700 ℃焙烧的样品中已出现了新复合氧化物CeTi2O6的晶相峰, 随焙烧温度的升高, 此晶相峰也变得更加明显, 这说明高温焙烧有利于Ce与Ti发生固相反应而形成CeTi2O6结构; Raman结果表明, 焙烧后的Ce0.5Ti0.5O2并不是简单的TiO2和CeO2的复合, 而是形成了新的晶相结构, 这也进一步验证了CeTi2O6结构的生成.     

溶胶-凝胶法合成超细Li_(2 x)RE_xSi_(1-x)O_3及其离子导电性

用溶胶 凝胶法合成了Li2 xRExSi1 -xO3(RE =Pr ,Nd ,Sm ,Gd ;x =0～ 0 15 ) ,用DTA TG ,XRD ,TEM及交流阻抗等技术对样品的结构、形貌、粒径及离子导电性等进行了观察和测试。其固溶体形成范围是 0 相似文献   

Mn_xCo_(2.5-x)Al_(0.5)O_4尖晶石型三元复合氧化物催化分解N_2O(英文)

用溶胶凝胶法制备了一组Mn_xCo_(2.5-x)Al_(0.5)O_4尖晶石型三元复合氧化物,用于有氧气氛下的N_2O催化分解反应.用N_2物理吸附、X射线衍射(XRD)、扫描电镜(SEM)、H_2程序升温还原(H_2-TPR)、O_2程序升温脱附(O_2-TPD)、X射线光电子能谱(XPS)等技术对催化剂进行了结构表征,考察了催化剂组成、母液pH、K负载量等制备参数对其催化活性的影响.结果表明:K的加入弱化了催化剂表面的金属-氧化学键,有利于表面氧物种的脱除,改性催化剂有较高的催化活性和抗水性,其中母液pH=2、K/(Mn+Co)比为0.02的K/Mn_(0.2)Co_(2.3)Al_(0. 5)O_4催化剂活性较高,该催化剂在有氧、有氧有水气氛400℃连续反应50 h,N_2O转化率分别达98.5%和76.5%.     

Sn0.5Ti((0.5)O2固溶体的溶胶-凝胶法制备、表征及其热稳定性研究

采用溶胶-凝胶法制备了Sn_0.5Ti_0.5O₂固溶体.用X射线衍射(XRD)、差热分析(DTA)和红外(IR)技术对材料的结构和热稳定性进行了分析表征.固溶体的热稳定性与起始反应温度有关,在40℃水浴温度下制备的凝胶经1000℃烧结,发生了相分解,出现了富Sn和富Ti相,而在80℃水浴温度下制备的凝胶经1200℃烧结也不发生相分解,仍以Sn_0.5Ti_0.5O₂相存在,而且用差热分析也得到了同样的结论.     

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.     

Al掺杂La10(SiO4)6O3的制备及其导电性能

以溶胶-凝胶法在850℃制备了Al掺杂La10(SiO4)6O3,即La10(SiO4)6-x(AlO4)xO3-0.5x(x=0,0.5,1.0,1.5和2.0),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Al掺杂0.5时La10(SiO4)5.5(AlO4)0.5O2.75的电导率最大,在700℃时其电导率达到1.88×10-2S·cm-1。氧分压对电导率的研究表明,其主要的电荷载体是O2-离子。     

An X-ray and neutron powder diffraction study of the Ca2+xNd8−x(SiO4)6O2−0.5x system

The variation in lattice parameters with bulk composition and preparation temperature has been determined from X-ray powder diffraction data for the system Ca_2+xNd_8?x(SiO₄)₆O_2?0.5x. The structures of two members of this system have been further refined from time-of-flight neutron powder diffraction data using the Rietveld method. Both structures belong to the $\text{P6}{}_3\text{m}$ space group and are isomorphous with natural apatite, Ca₁₀(PO₄)₆(F, OH)₂. Samples prepared at 1250°C exhibit an ordered distribution of Ca and Nd cations between two nonequivalent sites. The room temperature lattice parameters of Ca₂Nd₈(SiO₄)₆O₂ are a = 9.5291(5)Å and c = 7.0222(1) Å, while those of Ca_2.2Nd_7.8(SiO₄)₆O_1.9 are a = 9.5303(4) Å and c = 7.0147(1) Å. The composition of the latter member is believed to represent the upper limit of solid solution for this system at 1250°C.     

Synthesis of Bi2O3 and Bi4(SiO4)3 Thin Films by the Sol-Gel Method

Bi2O3 thin films were prepared by dipping silica slides in ethanolic solutions of tris(2,2-6,6-tetramethylheptane-3, 5-dionato)bismuth(III) [Bi(dpm)3] [1] and heating in air at temperatures 500°C. Bi4(SiO4)3 homogeneous thin films were obtained from the reaction of the bismuth oxide coating with the silica glass substrate at temperatures higher than 700°C. For heat treatments at temperatures between 600°C and 700°C, Bi2SiO5 coatings were obtained. The composition and microstructure evolution of the films were determined by Secondary Ion-Mass Spectrometry (SIMS), X-Ray Photoelectron Spectroscopy (XPS) and Glancing Angle X-Ray Diffraction (GA-XRD). The synthesis procedure was reproducible and allowed the control of the Bi2O3 phase composition. Moreover, the thin film annealing parameters were correlated with the formation of bismuth silicates, among which Bi4(SiO4)3 (BSO) is very appealing for the production of fast light-output scintillators [2].     

Study of the ionic conductivity of Ca6La4(PO4)2(SiO4)4F2 and Ca4La6(SiO4)6F2

In order to enhance our knowledge about the Ca_10−xLa_x(PO₄)_6−x(SiO₄)_xF₂ (0 ≤ x ≤ 6) series, whose chemical stability decreases as the substitution degree increases, Ca₆La₄(PO₄)₂(SiO₄)₄F₂ and Ca₄La₆(SiO₄)₆F₂ compounds were prepared through a solid-state reaction. Their ionic conductivity was measured by impedance spectroscopy. The results indicate that the conductivity increases with substitution, and fits the Arrhenius equation over the investigated temperature range. At high temperatures, a change in the activation energy has been observed, which has been related to the nature of the Ca/La–F bond, i.e. to the polarizability of lanthanum.