Mahindra Ecole Centrale, Survey no: 62/1A, Bahadurpally Jeedimetla, Hyderabad, 500043, Telangana, India.
Department of Physics, National Sun Yat-Sen University, Kaohsiung, 804, Taiwan.
Sci Rep. 2017 Jul 3;7(1):4501. doi: 10.1038/s41598-017-04543-6.
Scientific efforts are growing to understand artificial BiFeO/SrRuO/SrTiO-heterostructures, wherein an altered environment at each interface, caused by epitaxial strains, broken symmetry, off-stoichiometry and charge transfer, can generate a rich spectrum of exotic properties. Herein, (BiPb)FeO/SrRuO/SrTiO-heterostructures were sputtered with various top (BiPb)FeO-layers at different growth temperatures (T ). Strain relaxation at each interface changes with T and generates an additional peak alongside with (BiPb)FeO at a high T of 700 °C. Rutherford backscattering (RBS) was employed to understand this unusual behavior as to whether it is a mixture of two phases, layer splitting or inter-diffusion of elements. Surprisingly, complete overlapping of random and aligned RBS spectra from the sample with T = 700 °C indicates the presence of a large amount of defects/distortions at the interfaces. The RBS compositional analysis gives clear evidence of Fe and Ru vacancies to an extent that the structural integrity may not be maintained. This abnormal condition can be explained by the inter-diffusion of Pb and Bi elements into whole films and even into the top layer of the SrTiO substrate, which compensates for these vacancies by substitutional replacement and is responsible for the generation of the additional SrTi(BiPb)O-peak. Below T , the magnetic properties change significantly with T .
科学研究正在努力深入了解人工 BiFeO/SrRuO/SrTiO 异质结构,其中各界面处的环境因外延应变、对称破缺、非化学计量比和电荷转移而发生改变,会产生丰富的奇异性质。在此,采用不同生长温度 (T) 的多种顶部 (BiPb)FeO 层对 (BiPb)FeO/SrRuO/SrTiO 异质结构进行了溅射。各界面的应变弛豫随 T 而变化,并在 700°C 的高温 T 下生成一个额外的 (BiPb)FeO 峰。卢瑟福背散射 (RBS) 用于研究这种异常行为,以确定其是否是两相混合物、层分裂还是元素的互扩散。令人惊讶的是,T = 700°C 时样品的随机和对齐 RBS 光谱完全重叠表明界面处存在大量缺陷/变形。RBS 成分分析清楚地证明了 Fe 和 Ru 空位的存在程度,结构完整性可能无法维持。这种异常情况可以通过 Pb 和 Bi 元素扩散到整个薄膜甚至 SrTiO 衬底的顶层来解释,通过替代置换来补偿这些空位,并导致额外的 SrTi(BiPb)O 峰的产生。在 T 以下,磁性性质随 T 显著变化。