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机构地区:[1]华东师范大学物理系,上海200062 [2]中国科学院上海技术物理研究所红外物理国家重点实验室,上海200083
出 处:《功能材料》2003年第6期687-689,共3页Journal of Functional Materials
基 金:国家自然科学基金资助项目(60223006);上海市青年科技启明星计划资助项目(02QD14053)
摘 要: 采用组合靶,利用射频磁控溅射在260℃的(111)Si片上面制备了不同Ni、La含量比的La Ni O薄膜。测试分析结果表明,在La含量较高时,薄膜为无定型结构,并且具有较大的电阻率。当Ni和La含量比>1∶1.44后,薄膜具有(100)择优取向的赝立方钙钛矿结构,同时具有金属导电特性。随着La过量的减少,晶面间距和面电阻都减小的很快,在Ni和La比例达到1∶1时,电阻率达到了最小值6.4Ω·μm,晶面间距也达到最小值0.389nm。随着Ni过量的增加,晶面间距和面电阻又逐步增大。在Ni过量较多时导致了NiO相和LNO(110)取向的出现。在晶面间距相同时,相对于La,Ni含量的过剩对薄膜导电性能具有较大的影响。文中对实验现象从LaNiO3薄膜的导电机理出发给出了比较合理的解释。La-Ni-O thin films of different La and Ni concentration ratios were deposited on the (111)Si at a substrate temperature of 260℃ by a rf-magnetron sputtering system with a combined target. Results shows that the film is of amorphous structure when La content was too high. The film was with (100) preferred orientation and metallic electric conduction as the atomic concentration ratio of La to Ni was less than 1.44∶1. When the composition gets the stoichiometric composition (Ni∶La=1:1), the lattice constant and the sheet resistivity of the film reaches their minimums as 0.389nm and 6.4Ω·μm respectively. Then, as excessiveness of Ni increases, NiO phase appears and LaNiO_3(110) orientation is observed. The results also demonstrated that the excessiveness of Ni affected the conductivity more than that of La at the same lattice constant. A practicable explanation also was provided according to the conducting mechanism of LaNiO_3.
关 键 词:磁控溅射 La-Ni-O薄膜 制备 导电性 晶格常数
分 类 号:TM22[一般工业技术—材料科学与工程]
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