Concomitant appearance of conductivity and superconductivity in (111) LaAlO3/SrTiO3 interface with metal capping

被引:3
作者
Bisht, R. S. [1 ]
Mograbi, M. [1 ]
Rout, P. K. [1 ]
Tuvia, G. [1 ]
Dagan, Y. [1 ]
Yoon, Hyeok [2 ,3 ]
Swartz, A. G. [2 ,3 ]
Hwang, H. Y. [2 ,3 ]
Li, L. L. [4 ,5 ]
Pentcheva, R. [4 ,5 ]
机构
[1] Tel Aviv Univ, Sch Phys & Astron, IL-6997801 Tel Aviv, Israel
[2] Stanford Univ, Dept Appl Phys, Geballe Lab Adv Mat, 476 Lomita Mall, Stanford, CA 94305 USA
[3] SLAC Natl Accelerator Lab, Stanford Inst Mat & Energy Sci, Menlo Pk, CA 94025 USA
[4] Univ Duisburg Essen, Dept Phys, Lotharstr 1, D-47057 Duisburg, Germany
[5] Univ Duisburg Essen, Ctr Nanointegrat Duisburg Essen CENIDE, Lotharstr 1, D-47057 Duisburg, Germany
基金
美国国家科学基金会;
关键词
2-DIMENSIONAL ELECTRON-GAS; OXIDE; FERROMAGNETISM; LAALO3;
D O I
10.1103/PhysRevMaterials.6.044802
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
In epitaxial polar-oxide interfaces, conductivity sets in beyond a finite number of monolayers (ML). This threshold for conductivity is explained by accumulating sufficient electric potential to initiate charge transfer to the interface. Here we experimentally and theoretically study the LaAlO3/SrTiO3 (111) interface where a critical thickness t(c) of nine epitaxial LaAlO3 ML is required to turn the interface from insulating to conducting and even superconducting. We show that t(c) decreases to 3 ML when depositing a cobalt overlayer (capping) and 6 ML for platinum capping. The latter result contrasts with the (001) interface, where platinum capping increases t(c) beyond the bare interface. Our density functional theory calculations with a Hubbard U term confirm the observed threshold for conductivity for the bare and the metal-capped interfaces. Interestingly, conductivity appears concomitantly with superconductivity for metal/LaAlO3/SrTiO3 (111) interfaces, in contrast with the metal/LaAlO3/SrTiO3 (001) interfaces where conductivity appears without superconductivity. We attribute this dissimilarity to the different orbital polarization of e(g)' for the (111) versus d(xy) for the (001) interface.
引用
收藏
页数:8
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aps.org, US, DOI [10.1103/PhysRevMaterials.6.044802, DOI 10.1103/PHYSREVMATERIALS.6.044802]
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