首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 78 毫秒
1.
共沉淀法合成制备Ce^3+掺杂Lu3Al5O12纳米粉体   总被引:2,自引:0,他引:2  
用碳酸氢铵作为沉淀剂,将硝酸镥、硝酸铝和硝酸铈配成混合溶液,采用反滴定共沉淀及低温煅烧前驱体的方法制备 Lu3Al5O12(Ce)纳米发光粉体.采用热分析(TG-DTA)、傅立叶红外光谱(FTIR)、X射线衍射(XRD)、透射电镜(TEM)和光致发光(PL)等分析测试方法对Lu3Al5O12(Ce)粉体制备过程中的物理化学变化及粉体的激发发射发光性能进行了研究.结果表明,采用反滴定共沉淀法制备工艺,经过1000℃煅烧2h,可以得到晶粒尺寸为30nm左右,仅有轻微团聚,单一石榴石相的Lu3Al5O12(Ce)粉体.并且在1000℃处理得到的粉体的光致发光最强.  相似文献   

2.
研究了共沉淀法制备Eu3+掺杂氧化镥(Lu2O3)发光粉体过程中三种不同的沉淀剂(氨水、碳酸氢铵以及NH3·H2O+NH4HCO3两者的混合溶液)对所得粉体形貌的影响. 通过差热热重质谱联用(DTA-TG-MS)和红外光谱研究了不同沉淀剂所得沉淀前驱体的热分解行为, 结合显微结构观察、粒度分布和比表面积测试, 对三种沉淀剂影响Lu2O3晶粒尺寸和团聚状态的规律进行了探讨. 研究发现: 采用NH3·H2O+NH4HCO3混合沉淀剂得到的Lu2O3粉体具有最佳的显微结构和粒径分布状态, 沉淀前驱体经1000℃煅烧2h, 粉体的平均晶粒尺寸为35nm, 中位粒径(D50)为0.48μm.  相似文献   

3.
用高纯Al粉体和Y2O3粉体(Al-Y2O3粉体)为原料采用固相反应法制备了YAG陶瓷. Al-Y2O3粉体高能经过球磨, 煅烧生成YAG粉体, 再真空烧结制备高致密YAG陶瓷. 采用DTA-TG对球磨Al-Y2O3粉体进行分析, 采用XRD、SEM对球磨的Al-Y2O3粉体、YAG粉体及YAG陶瓷进行了表征. 实验表明: Al-Y2O3粉体在~569℃时, Al粉强烈氧化, 并与Y2O3粉反应, 600℃煅烧出现YAM相, 随煅烧温度升高出现YAP相, 1200℃煅烧生成YAG粉体. 成型YAG素坯在1750℃保温2h真空烧结出YAG相陶瓷, YAG陶瓷相对密度可达98.6%, 晶粒生长均匀, 晶粒尺寸为810μm.  相似文献   

4.
采用湿化学共沉淀法合成了Nd3+掺杂的氧化镥纳米晶粉体, 研究了三种不同沉淀剂(NH4OH、NH4HCO3、NH4OH+NH4HCO3)对Nd3+∶Lu2O3纳米晶粉体性能的影响. 采用NH4OH+NH4HCO3混合溶液作复合沉淀剂所得粉体具有比表面积高(13.37m2/g)、颗粒尺寸小(~30nm)、粒度分布窄(60~160nm)的优点. 该粉体经过干压和等静压成型后, 素坯从室温至1400℃获得的线性收缩率可达17%, 其烧结活性明显高于其它两种沉淀剂所得的粉体. 在流动H2气氛下, 经1880℃/8h烧结可获得具有优良光学透明性的Nd3+∶Lu2O3透明陶瓷, 在1080nm波长处的直线透过率超过75%.  相似文献   

5.
以[AlO4Al12(OH)24(H2O) 127+(简写为Al13)溶液为铝源, 采取湿化学的方法合成尖晶石及尖晶石氧化锆复合粉体. 采用27Al NMR、DSC-TG、XRD和FTIR等研究前驱体结构、反应过程及微结构演变. 将氯化镁、氢氧化钠混合研磨后加入Al13溶液中, 得到由Mg6Al2CO3(OH)16·4H2O 和 β-Al(OH)3组成的前驱体, 经过600℃煅烧形成尖晶石, 更高温煅烧产物仍为尖晶石单相. 以Al13、MgCl2·6H2O和ZrOCl2·8H2O为原料制备的前驱体经600℃煅烧, 同样获得尖晶石和四方相氧化锆. Al13粉末和尖晶石氧化锆复合粉体的FTIR谱显示, 归属于[AlO6]的吸收谱带由608cm-1移至 601cm-1, 归属于 [AlO4] 的吸收谱带由761cm-1 移至 723cm-1. 前驱体中形成的AlOMg键合是以Al13为铝源合成尖晶石和尖晶石氧化锆复合粉体具有低温合成的主要原因.  相似文献   

6.
以Ni(NO3)6H2O、Al(NO3)3·9H2O、ZrOCl8H2O和Ce(NO3)6H2O为原料,采用共沉淀法分别制备了NiO/CeO2/γ-Al2O3和NiO/CeO2-ZrO2/Al2O3催化剂.通过X射线衍射(XRD)、透射电子显微镜(TEM)和近边X射线吸收精细结构(XANES)等方法对催化剂的组成结构进行表征.结果表明,煅烧温度高于600℃时,NiO/CeO2/γ-Al2O3催化剂中的NiO与γ-Al2O3载体发生作用,形成NiAl2O4尖晶石;而NiO/CeO2-ZrO2/Al2O3催化剂中,NiO能够稳定存在,没有NiAl2O4尖晶石生成,且Al2O3与CeO2和ZrO2作用形成一种新的Zr0.30Ce0.45Al0.25O1.87固溶体.  相似文献   

7.
Al_2O_3含量对Al_2O_3/LiTaO_3复合陶瓷介电性能的影响   总被引:1,自引:0,他引:1  
采用热压烧结法制备了Al2O3/LiTaO3 (ALT) 陶瓷复合材料, 研究了Al2O3不同体积含量(5vol%、10vol%、15vol%和20vol%)对LiTaO3压电陶瓷介电性能的影响. 结果表明:随着频率的增加, 不同Al2O3含量的ALT陶瓷复合材料的介电常数和介电损耗均降低, 但降低的幅度不同. 少量Al2O3(5vol%)的添加既能增大材料的介电常数同时又降低了材料的介电损耗, 但是随着Al2O3含量的继续增加, ALT陶瓷复合材料的介电常数和介电损耗都增大, 其居里温度先升高后降低. Al2O3作为第二相不但能促进LiTaO3陶瓷烧结致密,而且对ALT陶瓷复合材料的介电性能也有提高.  相似文献   

8.
石涛  周箭  申乾宏  杨辉 《无机材料学报》2009,24(6):1105-1109
采用溶胶凝胶法在硅衬底上制备了Al2O3∶Tb3+薄膜; 并采用DTA-TG、XRD、SEM、AFM及光致发光光谱对其进行了一系列表征; 分析了Al2O3∶Tb3+薄膜的发光机理, 探讨了热处理温度和Tb3+掺杂浓度对发光性能的影响规律. 研究结果表明, 采用溶胶凝胶法制备工艺, 制备了高发光强度的Al2O3∶Tb3+薄膜, 薄膜的最佳激发波长为240nm, Tb3+的最佳掺杂浓度为5mol%(Tb2O3/Al2O3=5mol%), 在240nm光激发下, 最强的发射峰出现在544nm附近; 并且制备的Al2O3∶Tb3+薄膜表面致密、平整且无裂纹产生, 表面粗糙度约为1.3nm, 有利于硅基光电子器件的制备和应用.  相似文献   

9.
以硝酸氧锆[ZrO(NO3)2·5H2O]和钨酸铵(H40N10O41W12·xH2O)为原料,采用共沉淀法合成了低热膨胀的ZrO2-ZrW2O8复合陶瓷, 着重研究了不同热处理条件对前驱体转变为ZrO2-ZrW2O8复合陶瓷的影响, 并探讨了前驱体生成及其转变的反应历程. 通过X射线衍射仪(XRD)、热重-差示扫描量热(TG-DSC)、扫描电子显微镜(SEM)、热膨胀仪等分析手段对样品的晶体结构、物相转变、断面微观形貌和热膨胀性能进行表征. 结果表明: 采用共沉淀法制备的前驱体在1150℃热处理2h可以合成高纯度、混合均匀的ZrO2-ZrW2O8复合陶瓷; 随烧结时间的延长, ZrW2O8衍射峰半高宽逐渐减小, 晶粒在不断长大; ZrO2-50wt%ZrW2O8复合陶瓷在30~600℃内的平均热膨胀系数为-3.2295×10-6K-1.  相似文献   

10.
复合钙钛矿氧化物La1-xSrxCo1-yFeyO3-δ是一种适于中温固体氧化物燃料电池的阴极材料. 采用柠檬酸螯合法合成了La0.6Sr0.4Co0.2Fe0.8O3-δ粉体, 并通过XRD和SEM, 研究了前驱体溶液pH值和煅烧温度对其粉体晶相结构的影响; 同时, 通过烧结体的SEM和交流阻抗分析, 详细讨论了前驱体溶液pH值和烧结温度对烧结体显微结构和阻抗特性的影响. 结果表明, 前驱体溶液pH=4、煅烧温度为900℃的粉体, 1400℃下烧结2h获得的烧结体, 具有最低的阻抗.  相似文献   

11.
K. Zhao  J.F. Feng  H. Li 《Thin solid films》2005,476(2):326-330
La0.67Ca0.33MnO3 (LCMO)/La0.67Sr0.33CoO3 (LSCO)/LCMO trilayer films are fabricated on single-crystal substrates NdGaO3 (110) and the interlayer coupling are investigated. Compared with LCMO single layer, sandwiches showed the enhanced metal-insulator transition temperature of LCMO layers. The magnetoresistance is dependent on spacer thickness and the peak value dramatically decreases when LSCO layer is thick enough because of shorting by the LSCO layer. The magnetic coercivity HC shows a nonmonotonic behavior with changing spacer layer thickness and the waist-like hysteresis indicates that there is an indirect exchange coupling between the top and bottom LCMO layers across the spacer layer.  相似文献   

12.
The varistor properties of the ZnO-Pr6O11-CoO-Cr2O3-Y2O3-In2O3 ceramics were investigated for different concentrations of In2O3. The increase of In2O3 concentration slightly increased the sintered density (5.60-5.63 g/cm3) and slightly decreased the average grain size (3.4-2.9 μm). The breakdown field increased from 6023 to 14822 V/cm with increasing concentration of In2O3. The nonlinear coefficient increased from 17.6 to 44.6 for up to 0.005 mol%, whereas the further doping caused it to decrease to 36.8. In2O3 acted as an acceptor due to the donor concentration, which decreases in the range of 1.02 × 1017 to 0.24 × 1017/cm3 with increasing concentration of In2O3.  相似文献   

13.
Hollandite-type compounds, Rb2Cr8O16, K2Cr2V6O16 and K2V8O16, were synthesized under high P-T conditions up to 1200°C and 7GPa. The structural refinement using a single crystal of Rb2Cr8O16 confirms that the structure is similar to that of K2Cr8O16. Magnetic measurements indicate that Rb2Cr8O16 is ferromagnetic below 295K, K2Cr2V6O16 paramagnetic down to 77K and K2V8O16 has susceptibility anomaly at 175K. These compounds are all semiconductive and show discontinuities in temperature-resistivity curves at points corresponding to magnetic anomalies.  相似文献   

14.
Transparent glasses in the system (100−x)Li2B4O7x(SrO---Bi2O3---Nb2O5) (10≤x≤60) (in molar ratio) were fabricated by a conventional melt-quenching technique. Amorphous and glassy characteristics of the as-quenched samples were established via X-ray powder diffraction (XRD) and differential thermal analyses (DTA) respectively. Glass–ceramics embedded with strontium bismuth niobate, SrBi2Nb2O9 (SBN) nanocrystals were produced by heat-treating the as-quenched glasses at temperatures higher than 500 °C. Perovskite SBN phase formation through an intermediate fluorite phase in the glass matrix was confirmed by XRD and transmission electron microscopy (TEM). Infrared and Raman spectroscopic studies corroborate the observation of fluorite phase formation. The dielectric constant (r) and the loss factor (D) for the lithium borate, Li2B4O7 (LBO) glass comprising randomly oriented SBN nanocrystals were determined and compared with those predicted based on the various dielectric mixture rule formalism. The dielectric constant was found to increase with increasing SBN content in LBO glass matrix.  相似文献   

15.
Phase equilibria along the PbSbBiS4-Sb2S3 and PbSbBiS4-Bi2S3 joins of the PbS-Sb2S3-Bi2S3 system have been studied for the first time using differential thermal analysis, X-ray diffraction, microstructural analysis, microhardness tests, and density measurements, and the phase diagrams of the joins have been mapped out. The joins are shown to be pseudobinary with limited series of terminal solid solutions. The solid solutions are p-type semiconductors.  相似文献   

16.
Epitaxial YBa2Cu3O7/La0.7Ca0.3MnO3 (YBCO/LCMO) bi-layers and La0.7Ca0.3MnO3/YBa2Cu3O7 (LCMO/YBCO) bi-layers were grown on (001)LaAlO3 by pulsed laser deposition, and their microstructures were compared by transmission electron microscopy investigation. In the YBCO(100 nm)/LCMO(150 nm) bi-layers, the LCMO layer consists of columnar grains of ~ 17 nm in diameter and contains mixed orientation domains of [100]c, [010]c and [001]c. The YBCO layer is totally c-axis oriented and the YBCO lattices are tilted − 2.5° to + 2.5° as they grew on the rough surfaces of LCMO columnar grains. For the LCMO(140 nm)/YBCO(140 nm) bi-layers, the LCMO/YBCO interface is sharp and flat. The initial 12-nm thickness of the YBCO layer is composed of c-axis oriented domains, and the upper part of YBCO layer is [100] oriented. The LCMO layer was predominantly [001]c oriented while [100]c-oriented domains were occasionally observed.  相似文献   

17.
Sr0.3Ba0.7Nb2O6 (SBN) and La0.030Sr0.255Ba0.700Nb2O6 (LSBN) ceramic compounds have been prepared using the traditional ceramic method at two different calcination temperatures (900 and 1000 °C) and later sintered both at 1400 °C. A study of the effects of the calcination temperatures and La substitution on the morphological, compositional, and structural properties of SBN and LSBN is presented using scanning electronic microscopy (SEM), energy dispersive spectroscopy (EDS), and X-ray diffraction (XRD) analysis. From Rietveld refinement processes, the XRD patterns were interpreted to evaluate such effects in the structural parameters and the site occupation factors of the heavy metals and oxygen atoms. The effect of the incorporation of La resulted in a 0.25% cell contraction and turned out to be higher than the 0.08% dilation effect produced by the increase of calcination temperature. The La ion with similar effective ionic radius and higher electronegativity is incorporated into the structure occupying the A1 site just like the Sr ions in the SBN compound. Differences in the site occupation factors between the SBN and LSBN samples lead to substantial changes in the physical properties such as temperature of relative dielectric constant maximum, relative dielectric constant, and dielectric loss, correlated with the distortion and the relative orientation of the oxygen octahedra.  相似文献   

18.
We investigated the structural and superconducting properties ofc-axis oriented (YBa2Cu3O7) nY /(PrBa2Cu3O7) npr superlattices with thicknesses of the individual layers down to one unit cell (10nY1; 18>nPr 1). By transmission electron microscopy and X-ray diffraction we find an excellent structural quality of the samples, though the quantitative analysis shows the existence of defects. In superlattices with decoupled YBa2Cu3O7 layers of two unit cell thickness we find a highT c value of 75 K. We probed the flux line structure in the superlattices by measurements of the critical current density in magnetic fields. The experiments show that the flux-line dynamics is dominated by the movement of pancake vortices.  相似文献   

19.
A systematic study was performed with mixtures consisting of N2, CH4, C2H6 and C3H8, to investigate experimentally phase equilibria and caloric properties and to test the accuracy of thermodynamic correlations. The first part of this Paper reports results of T---p---x---y measurements on ternary systems in the range 20 < p < 120 bar and 140 < T < 220 K. The results are compared with data calculated by generalized equations of state.  相似文献   

20.
戴剑锋  田西光  闫兴山  李维学  王青 《材料导报》2017,31(22):30-34, 59
采用静电纺丝技术制备出表面光滑、直径均匀的Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4/PVP和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4/PVP纳米纤维前驱丝,经500~900℃煅烧后得到Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维。用TG-DSC、XRD、SEM及VSM现代测试分析手段对Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的结构、形貌及磁学性能进行测试表征。结果表明:在空气气氛中经500~900℃煅烧后可得到纯尖晶石相、结晶度良好的纳米纤维或短纤维;当温度为700℃时,Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的形貌细长而光滑且直径相对均匀,大约为80nm;此时Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4纳米纤维则保有较高的剩磁比(M_r/M_s)及矫顽力,分别为0.56和1 088.87Oe。在500℃、600℃、700℃、800℃、900℃煅烧后,Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的饱和磁化强度分别比Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4纳米纤维增大了14.5%、7%、16%、10.7%、8%,而矫顽力则分别降低了38%、51%、50%、46%、46.7%。两种纳米纤维的饱和磁化强度及矫顽力存在差异,为CoNi铁氧体在电磁方面的应用提供了很好的参考。  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号