溶胶-凝胶法引入ZnO-2B2O3-7SiO2玻璃对BaO-Sm2O3-4TiO2陶瓷性能的影响

采用固相反应法合成BaO-Sm2O3-4TiO2 (BST)陶瓷粉体.系统研究了溶胶-凝胶法引入ZnO-2B2O3-7SiO2 (ZBS)玻璃对BST陶瓷烧结特性、物相组成、微观形貌及介电性能的影响.结果表明,添加ZBS玻璃的陶瓷试样主晶相仍为类钙铁矿钨青铜结构的BaSm2Ti4O12,次晶相为Sm2Ti2O7.通过溶胶-凝胶法添加6％(质量分数)的ZBS玻璃,可使BST陶瓷的烧结温度从1350℃降低到1050℃,在1050℃烧结3h所得BST陶瓷介电性能优良:εr=60.17,tanδ=0.004,τf=-7.9×10 6/℃.     

低温烧结Ca0.6La0.8/3TiO3-Li0.5Nd0.5TiO3微波介质陶瓷

研究了复合烧结助剂ZnO-B2O3-SiO2(ZBS)玻璃和LiF添加量对Ca0.6La0.8/3TiO3-Li0.5Nd0.5 TiO3(CLLNT)陶瓷相结构、烧结特性及介电性能的影响.加入复合烧结助剂(ZBS玻璃和LiF)后,CLLNT陶瓷的烧结温度从1400℃降至1000℃;当ZBS玻璃的添加量为4%(质量分数,下同)、LiF的添加量小于3%时,CLLNT陶瓷样品中没有发现第二相,主晶相仍为斜方钙钛矿结构;当ZBS玻璃的添加量为4%、LiF的添加量为1%时,CLLNT陶瓷在1000℃烧结3h获得最佳性能,介电常数εr=97,Q×f=1286GHz,TCF=43×10-6/℃(4GHz).     

掺ZBS玻璃低温烧结ZnNb2O6微波介质陶瓷的研究

研究了ZnO-B2 O3-SiO2(ZBS)玻璃料对ZnNb2O6微波介质陶瓷烧结特性和介电性能的影响.结果表明,ZBS玻璃料形成的液相加速了颗粒间的传质,促进了烧结,能使ZnNb2O6陶瓷的烧结温度有效地降低至950℃.随着ZBS含量的增加,样品中出现了第二相,且气孔被包裹在晶粒内部难以逃脱出来,导致样品的缺陷和损耗增加,从而降低介电性能.掺杂1%ZBS的ZnNb2O6陶瓷在950℃保温4h,能获得优异的综合介电性能:ε=23.56、Q·f=18482GHz、τf=-28.8×10￣6/℃.     

Ba4(Nd0.85Bi0.15)28/3Ti18O54陶瓷低温化研究

采用复合添加BaCuO2-CuO和BaO-B2O3-SiO2助剂的方法,研究了Ba4(Nd0.85Bi0.15)28/3 Ti18O54陶瓷的低温烧结特性和微波介电性能.添加2.5wt?CuO2-CuO和5wt?O-B2O3-SiO2后Ba4(Nd0.85 Bi0.15)28/3 Ti18O54陶瓷在950℃烧结成瓷,气孔率为5.29%,介电常数ε为60.25,Q·f值为2577GHz(5.6GHz),频率温度系数τf为 25.1ppm/℃,可与Cu电极浆料低温共烧.     

复合添加La_2O_3/MgO对(Zr_(0.8)Sn_(0.2))TiO_4陶瓷性能的影响

讨论了复合添加La2O3/MgO对(Zr0.8Sn0.2)TiO4介质陶瓷烧结机制和微波介电性能的影响。结果表明,La2O3/MgO对(Zr0.8Sn0.2)TiO4的烧结有一定的促进作用,但La2O3/MgO添加量的增大会造成晶格缺陷和残留气孔的增多,从而导致材料的密度和Q×f降低。在1320℃保温12h、La2O3/MgO添加量为0.9wt%时,(Zr0.8Sn0.2)TiO4介电性能最好,其εr=37.14,Q×f=36600,τf=7.77×10-6/℃。     

(1-x)(Mg0.7Zn0.3)TiO3-xCa0.61La0.26TiO3系陶瓷的微波介电性能研究（英文）

本实验研究了(1-x)(Mg0.7Zn0.3)TiO3-x(Ca0.61La0.26)TiO3(MZT-CLT)系陶瓷的微观结构和微波介电性能,通过(Ca0.61La0.26)TiO3来协调(Mg0.7Zn0.3)TiO3陶瓷的谐振频率温度系数.MZT-CLT陶瓷的主晶相为(Mg0.7Zn0.3)TiO3,第二相为Ca0.61La0.26TiO3和(Mg0.7Zn0.3)Ti2O5.烧结温度和陶瓷组成对微波介电性能影响显著,当烧结温度为1275℃时,可以获得良好的致密度,当烧结温度超过1300℃时,Zn的蒸发导致陶瓷致密度和介电性能下降.随着(Ca0.61La0.26)TiO3含量的增大,材料的介电常数增大,品质因数减小.当x=0.13,烧结温度为1275℃保温4h,(MZT-CLT)陶瓷具有优良微波介电性能,εr=26,Q.f=86000 GHz,τf=-6×10-6/℃.     

原料粉体的引入方式对Li_2O-Nb_2O_5-TiO_2复合微波介质陶瓷结构及性能的影响

通过XRD、SEM等分析手段,结合介电性能测试结果,探讨了两种不同的原料粉体引入方式H1及H2,对Li2O-Nb2O5-TiO2陶瓷体系中"M-相"与Li2TiO3固溶体(Li2TiO3ss)共存的复合陶瓷材料(H1及H2陶瓷)的烧结行为、微观结构以及微波介电性能的影响。采用H2方式制备的H2陶瓷,1100℃烧结2h,材料具有较优异的微波介电性能:介电常数εr=40.2,Q×f值高达9900GHz,频率温度系数τf=4.6×10-6/℃,是一种性能优异的微波介质陶瓷材料。     

CaTiO3 对(1-x)ZnAl2O4-xMg2TiO4(x=0.21)微波介质陶瓷结构和性能的影响

利用常规固相法制备了ZnAl2O4-Mg2TiO4-CaTiO3陶瓷,研究了CaTiO3对其相成分、微观组织结构和微波介电性能的影响规律. 结果表明,CaTiO3能有效地改善(1-x)ZnAl2O4-xMg2TiO4(x=0.21)材料的烧结性能,使其致密化温度降低150℃. ZnAl2O4-Mg2TiO4-CaTiO3陶瓷体系中包括ZnAl2O4基尖晶石相、CaTiO3、MgTi2O5和Zn2Ti3O8相,当烧结温度高于1400℃时,Zn2Ti3O8相消失. 随着CaTiO3含量的增加,体系中CaTiO3相含量增加而MgTi2O5相含量减少,且CaTiO3具有显著地调节谐振频率温度系数的作用. 当在(1-x)ZnAl2O4-xMg2TiO4(x=0.21)体系中掺入6mol%的CaTiO3添加剂时,经1400℃烧结后能获得温度稳定性好的微波介质陶瓷材料,其微波介电性能为:εr=11.8,Q*f=88080GHz,τf=-7.8×10-6/℃.     

ZnO-MgO-TiO_2-SnO_2系高频介电陶瓷的制备与介电性能

在ZnO-TiO2-SnO2陶瓷基础上,掺杂MgO得到(1-x)ZnO-xMgO-0.88TiO2-0.12SnO2系新型介电陶瓷。对其相转变、微观组织结构和高频介电性能进行了研究,结果表明,在不加入任何烧结助剂情况下,试样可于1 080℃达到烧结,其相对密度为94.4%;当x=0.05时,陶瓷为纯相尖晶石结构(Zn0.95,Mg0.05)2(Ti0.88,Sn0.12)O4,其介电性能优良,1 MHz时ε=18.88,tanδ=5×10-4,τε=2.89×10-6/℃,可用作高频电容器材料的优秀候选材料。     

ZnO掺杂对CLST微波介质陶瓷烧结及介电性能的影响

研究了烧结助剂ZnO对CaO-Li2O-Sm2O3-TiO2(简写为CLST)系微波介质陶瓷的烧结特性及介电性能的影响.结果表明:ZnO的添加能有效地降低CLST陶瓷的烧结温度至1150℃.掺杂2wt%ZnO的CLST陶瓷取得了较好的介电性能:εr=84,tanδ=0.009,τf=-15ppm/℃.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Thermoelectric power of single-phase samples of Tl2CaBa2Cu2O y and Ba2CaSr2Cu2O y

Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-T _c . The thermopower was positive and decreased linearly with increasing temperature aboveT _c (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model.     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Structure of Na2O·2TiO2 glass

X-ray radial distribution analysis and Raman spectroscopic measurement were carried out on Na₂O-2TiO₂ glass prepared by twin-roller quenching method. It is found that four-coordinated Ti⁴⁺ ions may be predominant over six-coordinated ones in the present glass. It is also found that the fraction of six-coordinated Ti⁴⁺ ions is larger in the present glass than in K₂O·2TiO₂ and Cs₂O·2TiO₂ glasses. Poorer glass-forming ability of the Na₂O-TiO₂ system compared with the K₂O-TiO₂ and Cs₂O-TiO₂ systems is ascribed to a larger fraction of TiO₆ octahedron for the former system.     

SiO2—TiO2—ZrO2系涂层的制备及其特性

用溶胶－凝胶法（sol-gel method）在不锈钢表面制备了SiO2-TiO2-ZrO2系无机氧化膜（STZ）。用DTA／TG、IR、XRD和SEM等手段研究了涂层制备时由凝胶向玻璃态的转变以及涂层薄膜的显微结构特点，考察了涂层对基体的保护效果。试验结果表明，在溶胶至凝胶最终转变为无机氧化物的过程中形成了无机网络，Si^4 和Zr^4 充当了网络骨架的形成离子。涂层为无定型玻璃态，其间混有石英、锐钛矿或金红石等微晶。     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.     

Investigation of Instability of Lattice of Bi_2Sr_2CaCu_2O_x

Bi2Sr2CaCu2Ox superconductor was studied by differential scanning calorimetry (DSC) and thermogravimetry (TG) in different atmospheres. It is discovered that there is a thermal anomaly in the DSC curve, associated with a weight loss in the TG curve before the melting of the sample. Careful thermal analysis and high temperature X-ray diffraction reveal that the thermal anomaly and the weight loss show an instability of the crystalline Iattice. By annealing the sample in oxygen and argon, respectively and then by TC measurement and thermal analysis, the coincidence of transition temperature with the instability is found. The coincidence is further confirmed by Y-doped 2212 phase.     

Thermal conductivity of the system N2O4 ⇄ 2NO2 ⇄ 2NO + O2

Experimental data on the thermal conductivity of dissociating nitrogen tetroxide have been obtained by the hot-wire method in the temperature range from 290 to 870° K at pressures up to 10⁵ N/m².