离子束溅射法制备La0.5Sr0.5CoO3薄膜的拉曼光谱分析

采用离子束溅射在氧化钇稳定的氧化锆(YSZ)和铝酸镧(LaAlO3)上制备了La0.5Sr0.5CoO3的钙钛矿薄膜.利用拉曼光谱,研究了不同热处理温度和不同衬底对LSCO薄膜材料的晶体结构、分子振动模式和化学键的影响.研究发现La0.5Sr0.5CoO3钙钛矿薄膜的晶体结构随着热处理温度的升高发生明显的相变,由排列无规则态朝着正交晶系结构转变,Co-O键构成的八面体间的相对运动强度逐渐减弱.另外,还发现La0.5Sr0.5CoO3钙钛矿薄膜在衬底氧化锫(YSZ)上的Co-O键振动频率要小于在衬底铝酸镧(LaAlO3)上的振动频率,这与两者的品格失配程度有关.     

Ln0.5Sr0.5CoO3-δ阴极薄膜材料的XRD和XPS研究

采用离子束溅射法在氧化钇稳定的氧化锆(YSZ)衬底和铝酸镧(LaAlO3)衬底上溅射Ln0.5Sr0.5CoO3-δ(Ln=La ,Pr ,Nd )薄膜.测试了不同工艺制备的Ln0.5Sr0.5CoO3-δ薄膜的XRD谱和XPS谱,研究了不同衬底上Ln0.5Sr0.5CoO3-δ薄膜微结构及化学状态.结果表明,在YSZ 衬底上制备的Ln0.5Sr0.5CoO3-δ薄膜氧空位浓度相应的高于在LaAlO3衬底上的氧空位浓度,Nd0.5Sr0.5CoO3-δ /YSZ薄膜的氧空位浓度最高,有利于提高氧离子的输运性.     

固体氧化物燃料电池Ln0.5Sr0.5CoO3薄膜阴极材料电学性能研究

采用离子束溅射法在YSZ(110)衬底上制备Ln0.5Sr0.5CoO3(Ln=La,Pr)钙钛矿多晶薄膜,研究了载流子浓度、迁移率与温度的关系,分析了A位置稀土离子半径rA3+对电导率的影响.结果表明,在375K～667K温度范围内,La0.5Sr0.5CoO3薄膜的载流子浓度由4.76×1027/m3升高到9.43×1027/m3,迁移率由0.21cm2/Vs升高到0.218cm2/Vs;Pr0.5Sr0.5CoO3薄膜的载流子浓度由0.58×1027/m3升高到7.9×1027/m3,迁移率由0.0853cm2/Vs升高到0.172cm2/Vs.Ln0.5Sr0.5CoO3薄膜的霍尔系数激活能EH与电导激活能Eα的比值近似为2/3,符合Emin和Holstein的小极化子绝热区域导电理论.     

钙钛矿结构氧化物La_(0.5)Sr_(0.5)CoO_3的电导性能研究

采用固相反应法制备了La_(0.5)Sr_(0.5)CoO_3样品,利用X射线衍射仪和拉曼光谱仪对样品结构进行分析。XRD结果显示,La_(0.5)Sr_(0.5)CoO_3样品为单相的立方钙钛矿结构。拉曼光谱图中可看到由氧八面体旋转产生的谱峰以及由Co—O键角及键长振动形成的二级拉曼峰。利用第一性原理的方法计算了La_(0.5)Sr_(0.5)CoO_3的能带、态密度与分波态密度,结果表明Sr~(2+)的掺入可以使不导电的钙钛矿型氧化物LaCoO_3的导电性发生改变,这对钙钛矿型氧化物LaCoO_3的电导特性研究具有指导意义。     

Preparation and Electrical Transport Properties of Perovskite Oxide Ln0.5Sr0.5CoO3

The superfine powders of Ln0.5 Sr0.5 CoO3 （Ln = La, Pr, Nd, Sm, Eu） were obtained by solid state reactions. The crystal structure and electrical transport properties of samples doped with different rare earth elements as well as the forming process of the Perovskite structure were studied. The result shows that when the temperature reaches 1200 ℃, the samples will become a steady and unitary Perovskite phase by solid state reactions. The conductive behavor at low temperature is consistent with small polaron mechanism （i. e., localized electronic carriers having a thermally activated mobility）. However, the maximum of conductivity appears at about 700 ℃, and the conductivity of La0.5Sr0.5CoO3 is the biggest in the intermediate-temperature （600 - 850 ℃ ）, so it is fit for cathode material of intermediate-temperature solid oxide fuel cells.     

镧锶钴复合氧化物的水热合成与表征

以硝酸镧、硝酸锶、硝酸钴为金属源,柠檬酸为络合剂,采用水热法于180℃下保温24 h合成镧锶钴复合氧化物.XRD分析表明产物为斜方六面体钙钛矿结构的La0.8Sr0.2CoO3-δ晶相.SEM分析表明产物为球状颗粒,尺寸约0.5～1μm.红外吸收光谱表明产物主要为La0.8Sr0.2CoO3-δ,此外还残留部分柠檬酸和...     

(La1-xPrx) 2/3Sr1/3CoO3 的成相过程与电导性能研究

采用固相反应法合成了(La1-xPrx) 2/3Sr1/3CoO3 (x=0.2,0.4,0.6,0.8) 双稀土氧化物系列粉体,研究了(La0.6Pr0.4) 2/3Sr1/3CoO3的成相过程和电导性能.结果表明,在实验过程中首先出现了La2O(CO3)和La2SrOx相,而La2SrOx相在270℃～910℃的较大范围内一直存在,再经过两次吸热到910℃时出现了(La0.6Pr0.4) 2/3Sr1/3CoO3 晶相,当温度达到1000℃时,(La0.6Pr0.4) 2/3Sr1/3CoO3 成为主晶相,在1250℃下烧结2h后,样品已成单一钙钛矿结构(La0.6Pr0.4) 2/3Sr1/3CoO3相.(La1-xPrx)2/3Sr1/3CoO3(x=0.2,0.4,0.6,0.8)双稀土氧化物的电导率在700℃附近时出现最大值,其中(La0.8Pr0.2) 2/3Sr1/3CoO3的电导率在中温范围内最大,适合作为中温固体氧化物燃料电池阴极材料.     

Sm0.5-x Gdx Sr0.5CoO3-δ阴极材料的制备及其性能表征

采用固相法制备了钙钛矿型氧化物Sm0.5-xCdxSr0.5CoO3-δ(x =0,0.1,0.2,0.3,0.4,0.5)粉体.利用XRD分析材料的物相组成,用热膨胀仪测定了材料的热膨胀系数.利用交流阻抗法测试了Sm0.5-xGdxSr0.5CoO3-δ/SDC复合阴极的极化电阻.结果表明,粉体在1200℃热处理6h后形成正交钙钛矿型结构;从室温到800℃范围内,材料的平均热膨胀系数TEC为11.43×10-6℃-1～14.35×10-6℃-1,掺杂Gd3+以后Sm0.5-xGdxSr0.5CoO3-δ样品的热膨胀系数比Sm0.5Sr0.5 CoO3-δ样品的热膨胀系数略有增加.800℃时,复合阴极的极化电阻随x的增大先减小后增大,在x=0.1时,最小为0.05Ω;所有样品的极化电阻随测试温度的升高而降低.     

倾斜衬底上沉积的钙钛矿结构氧化物薄膜的电阻各向异性

用脉冲激光沉积法(PLD)分别在平的和倾角为10°、15°、20°的LaAlO3倾斜衬底上制备了La0 5Sr0 5CoO3薄膜和La0 67Ca0 33MnO3薄膜。用四探针法测量薄膜表面的电阻,发现平衬底上生长的薄膜没有电阻各向异性,而倾斜衬底上生长的薄膜存在电阻各向异性现象,并且倾角越大,电阻各向异性越明显。这是由于倾斜衬底上薄膜的自组织结构造成的。     

Magnetic Transition of La0.8Sr0.2Mn1-xCoxO3（x =0, 0.3, 0.5, 1.0）

A series of rare earth compound oxides with the formula of La0.8Sr0.2Mn1-xCoxO3（ were prepared by the method of citric acid. Structures, figures and magnetic properties of the x=0.0, 0.3, 0.5, 1.0） samples were analyzed by means of XRD, SEM and SQUID. Experiment results prove that all the samples are hexagonal, but their figures and magnetic properties are different. La0.8Sr0.2MnO3 is ferromagnetic. La0.8Sr0.2Mn0.7CO0.3O3 and La0.8Sr0.2Mn0.5Co0.5O3 are ferrimagnetic. La0.8Sr0.2CoO3 is antiferromagnetic. SEM results indicate that the structure of the first three are three-dimensional reticulations which are made up of some small ellipsoids which link up at the head and the end. The fourth sample looks like some dispersed small balls.     

Age Hardening of the Al0.5CoCrNiTi0.5 High-Entropy Alloy

Al_0.5CoCrNiTi_0.5 high-entropy alloy was synthesized by vacuum arc melting in a copper mold. This alloy was aged at 773 K to 1473 K (500 °C to 1200 °C) for 24 hours to investigate the microstructure and hardness. The hardness of the as-cast alloy is HV743, and it exhibits a dendritic structure, in which dendrite is composed of body-centered cubic (bcc), face-centered cubic (fcc), and σ phases, and interdendrite is an eutectic structure consisting of bcc and order bcc phases. Apparent age hardening appears at 873 K to 1173 K (600 °C to 900 °C), and no age softening occurs even after 1473 K (1200 °C) aging. The age hardening of this alloy is attributed to the transformation of the bcc phase to σ phase. Detailed variations of hardness and the microstructure of aged alloys are reported in this article.     

Crystallization and characterization of substoichiometric compound (W0.5Al0.5)C0.5 obtained by solid-state reaction

(W_0.5Al_0.5)C_0.5 substoichiometric compound is synthesized by a combination of mechanical milling and high-pressure reactive sintering. X-ray diffraction is used to monitor the phase changes and crystallization of (W_0.5Al_0.5) C_0.5 during the whole reaction process. As a result, (W_0.5Al_0.5) C_0.5 is identified as the hexagonal WC-type belonging to the P-6m2 space group (No. 187), and the lattice parameters of (W_0.5Al_0.5)C_0.5 are calculated to be a=2.907 (1) Å, c=2.838 (1) Å, which are very similar to those of WC even if there are approximately 50 pct carbon vacancies in the cell of (W_0.5Al_0.5)C_0.5 as compared with WC. The substoichiometric (W_0.5Al_0.5)C_0.5 compound has a Vickers microhardness of 2385±70 kg mm^?2, which is as high as that of WC, while its density is far lower than that of WC.