Tiron对纳米Al2O3悬浮液性能的影响

以1,2-二羟基苯-3,5-二磺酸钠(Tiron)为分散剂获得了平均粒径约为57nm的氧化铝粉体的稳定悬浮液.通过测定等温吸附曲线及悬浮液的Zeta电位,研究了Tiron对粉体表面特性的影响.结果表明,Tiron在Al₂O₃表面发生化学吸附,磺酸基的离解使胶粒表面电荷更负,显著提高颗粒表面的带电量,从而改善浆料的稳定性.FTIR研究表明:Tiron分子结构中两个相邻羟基与Al-OH形成内环结构,从而提高了吸附强度.流变测试确定了制备高固含量稳定浆料在pH=8.5时所需的最佳分散剂用量为0.8wt％.     

Y-TZP悬浮液的界面吸附特性

本文利用聚电解质分散剂聚丙烯酸铵（ＮＨ_４ＰＡＡ）制备了稳定的Ｙ－ＴＺＰ悬浮液．通过等温吸附实验和电动特性测定发现,分散剂浓度为２ｗｔ％时,在粉体颗粒表面的吸附达饱和,悬浮液的等电点（ＩＥＰ）向酸性区移动．扫描俄歇能谱（ＳＡＭ）分析和原子力显微镜（ＡＦＭ）研究表明,粉体的表面化学键结构因分散剂的吸附而改变,悬浮颗粒之间的相互排斥能增大．悬浮液的粘度在分散剂饱和吸附时达到最小值,浆料的悬浮稳定性得到了提高.     

BaTiO3颗粒对分散剂PMAA-NH4的吸附机制研究

通过ζ电位测量及PTIR分析，研究了BaTiO3颗粒对阴离子型分散剂PMAA－NH4的吸附机制。结果表明，加入PMAA－NH4后，由于BaTiO3颗粒表面上存在Ba-OH2^ 的正电荷中心，从而吸附了分散剂的阴离子，使BaTiO3表面带电特性改变，等电点由pH＝5.1移至pH=3.5，当pH=10，PMAA－NH4的加入量为0．8wt％时，BaTiO3颗粒表面吸附达到饱和，可以得到稳定性好的BaTiO3悬浮体。     

低毒单体DMAA用于ZrO2/Al2O3坯体注凝成型

采用低毒的单体N, N-二甲基丙烯酰胺(DMAA)制备了氧化锆增韧氧化铝(ZrO₂/Al₂O₃)坯体。讨论了分散剂的用量、 ZrO₂/Al₂O₃浆料的pH值、 粉体中ZrO₂含量、 粉体所占浆料的固相体积分数、 球磨时间、 预混液中DMAA的浓度(质量分数)对ZrO₂/Al₂O₃浆料黏度的影响。并研究了注凝成型ZrO₂/Al₂O₃坯体的性能和显微结构。结果表明, 当浆料pH值为9, 分散剂的添加量为ZrO₂/Al₂O₃粉体质量的0.6%, 球磨时间为6 h, ZrO₂/Al₂O₃浆料具有最小的黏度。固相体积分数的提高和DMAA加入量的增大都会提高ZrO₂/Al₂O₃浆料的黏度, ZrO₂的加入会降低浆料的黏度。用DMAA制备得到的ZrO₂/Al₂O₃坯体结构均匀, 抗弯强度达到25 MPa。      

水相体系纳米γ-Al2O3浆料的分散稳定性能研究

为确定配制稳定的纳米γ-Al2O3化学机械抛光(CMP)浆料的工艺条件,通过润湿性、Zeta电位及黏度的测定,研究了溶液pH值及添加分散剂等因素对水相体系纳米γ-Al2O3悬浮液分散稳定性能的影响.结果表明,在纳米γ-Al2O3固含量为6%的浆料中,加入异丙醇胺作为分散剂,其用量为γ-Al2O3粉体质量的1%,同时控制浆料的pH值约为4时,纳米γ-Al2O3粉末的润湿性能最佳,此时浆料Zeta电位值较高,黏度较小;在该条件下成功获得长时间不沉降的稳定浆料.     

Al2O3颗粒形貌对注凝成型ZrO2/Al2O3陶瓷性能的影响

采用3种不同形貌的Al₂O₃原料对注凝成型制备ZrO₂/Al₂O₃（ZTA）陶瓷工艺中悬浮体的流变性能进行了研究。以低毒的单体N,N-二甲基丙烯酰胺（DMAA）制备了ZrO₂/Al₂O₃坯体和陶瓷。讨论了3种不同形貌的Al₂O₃原浆料的分散剂用量、球磨时间和固含量对浆料流变性的影响。Al₂O₃粉体呈扁平状有利于降低浆料的黏度,Al₂O₃粉体呈棒状对生坯强度的提高有利。制得的3种ZrO₂/Al₂O₃坯体颗粒间结合紧密,抗弯强度分别达到21.45,19.87,25.90 MPa。Al₂O₃粉体呈颗粒状有利于最终陶瓷力学性能的提高,陶瓷的抗弯强度及断裂韧性分别为680 MPa和7.49 MPa·m^1/2,453.1 MPa和6.8 MPa·m^1/2,549.4 MPa和6.34 MPa·m^1/2。     

丙烯酸-丙烯酸酯共聚物对钛酸铋水悬浮液性质的影响

研究了丙烯酸－丙烯酸酯共聚物对钛酸铋（Bi4Ti3O12)悬浮液表面化学性质及流变性的影响。结果表明，共聚物的加入使Bi4Ti3O12的等电点向低pH值方向偏移。共聚物在粉体表面的吸附属于物理吸附，其含量的变化可以引起共聚物在粉体表面吸附构型的变化，当共聚物含量＞1．5wt%时，部分高分子脱附。共聚物的加入可以显著改善悬浮液的稳定性，在低共聚物含量和高共聚物含量均可制备稳定的悬浮液，共聚物含量≤1．5wt%时，浆料的稳定通过静电位阻稳定机理来实现，共聚物含量≥2.0wt%时，可能通过空位稳定机理来实现。     

温度对α-Al2O3-H2O-PAA悬浮液稳定性的影响

研究了温度对α-Al2O3 -H2O-聚丙烯酸悬浮液分散稳定性的影响.研究表明:温度升高,粉体充分分散时所需的PAA添加量增大.浆料体系中分散剂添加量低于给定温度下的最佳添加量时,温度升高,浆料粘度增加,稳定性下降.但在适量聚丙烯酸(polyacrylic acid,PAA)分散剂存在的前提下,提高温度,可以显著降低高固含量浆料的粘度.     

α-Al_2O_3稳定浆料的研究

本文研究了分散剂种类及数量、pH值等对大颗粒α－Al2O3陶瓷浆料稳定性的影响，得到了具有一定粘度和流动性适于制备α－Al2O3陶瓷膜管的稳定浆料．     

用于电泳沉积的TiO2悬浮液分散性能研究

为了制备适合电泳沉积用的稳定悬浮液,在TiO2水基悬浮液中添加了聚乙烯亚胺(PEI)作为分散剂,对TiO2水基悬浮液进行Zeta电位、黏度、粒径以及稳定性测试,研究了PEI分散剂对TiO2分散性能的影响.结果表明通过添加相对于悬浮液中TiO2粉体质量分数0.6%～3.0%的分散剂可以获得高稳定、高分散、低黏度的悬浮液.     

Varistor properties of ZnO-Pr6O11-CoO-Cr2O3-Y2O3-In2O3 ceramics

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.     

Nanocrystallization of SrBi2Nb2O9 from glasses in the system Li2B4O7---SrO---Bi2O3---Nb2O5

Transparent glasses in the system (100−x)Li₂B₄O₇–x(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.     

Characterization of YBa2Cu3O7/PrBa2Cu3O7 superlattices

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.     

Magnetic coupling in La0.67Ca0.33MnO3/La0.67Sr0.33CoO3/La0.67Ca0.33MnO3 sandwiches

La_0.67Ca_0.33MnO₃ (LCMO)/La_0.67Sr_0.33CoO₃ (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 H_C 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.     

The effect of Bi1.5Zn0.5Nb0.5Ti1.5O7 cover layer on the dielectric and tunable properties of Ba0.6Sr0.4TiO3/Bi1.5Zn0.5Nb0.5Ti1.5O7 bilayered thin films

Bi_1.5Zn_0.5Nb_0.5Ti_1.5O₇ (BZNT) thin films with different thicknesses as cover layers were deposited on the Ba_0.6Sr_0.4TiO₃ (BST) thin films on the Pt/Ti/SiO₂/Si substrates by radio frequency magnetron sputtering method. The microstructure, surface morphology, dielectric and tunable properties of BST/BZNT heterogeneous bilayered films were investigated as a function of the thickness of BZNT films and the effect of BZNT films on the asymmetric electrical properties of BST/BZNT bilayered films was discussed. It was found that BZNT cover layer significantly improved the leakage current and the dielectric loss, and the dielectric constant and tunability of BST/BZNT bilayered thin films simultaneously decreased with the increasing thickness of BZNT films. The BST/BZNT bilayered thin film with a 50 nm BZNT cover layer gave the largest figure of merit (FOM) of 33.48 with the upper tunability of 55.38%. The asymmetric electrical behavior of BST/BZNT bilayered films is probably related to an internal electric field caused by built-in voltages at Pt/BST and BZNT/Au interfaces.     

MoO3-V2O5-P2O5-Fe2O3玻璃的制备及性能研究

制备了MoO3-V2O5-P2O5-Fe2O3系磷酸盐玻璃,研究了玻璃形成能力、热膨胀系数和抗潮解等性能.结果表明,MoO3-V2O5-P2O5-Fe2O3系统具有较宽的玻璃形成区和较强的玻璃形成能力,当MoO3/V2O5≈1.5时,玻璃形成能力最强.MoO3-V2O5-P2O5-Fe2O3玻璃的热膨胀系数约为60～110×10-7/℃,并且随着Fe2O3含量的增加而逐渐增大.加入适量的Fe2O3能够显著改善MoO3-V2O5-P2O5玻璃的抗潮解性能,在90℃的去离子水中的溶解速率达到8.0×10-9g·cm-2·min-1.     

Structural study of Sr0.3Ba0.7Nb2O6 and La0.030Sr0.255Ba0.700Nb2O6 ceramic systems

Sr_0.3Ba_0.7Nb₂O₆ (SBN) and La_0.030Sr_0.255Ba_0.700Nb₂O₆ (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.     

Microstructures of YBa2Cu3O7/La0.7Ca0.3MnO3 and La0.7Ca0.3MnO3/YBa2Cu3O7 bi-layers grown on (001)LaAlO3

Epitaxial YBa₂Cu₃O₇/La_0.7Ca_0.3MnO₃ (YBCO/LCMO) bi-layers and La_0.7Ca_0.3MnO₃/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.     

Syntheses of hollandite type Rb2Cr8O16, K2Cr2V6O16 and K2V8O16

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.     

静电纺丝法制备的Co0.6Ni0.3Cu0.1Fe2O4和Co0.6Ni0.3Zn0.1Fe2O4纳米纤维的结构及磁性能

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。