Enhanced Superconductivity of La<sub>2-x</sub>Sr<sub>x</sub>CuO<sub>4</sub> Thin Films by Atomic-Scale Interface Engineering
ORAL
Abstract
Ruddlesden-Popper (RP) oxides (An+1BnO3n+1, n = 1, 2, ...) have been widely studied with tunable properties such as high-Tc superconductivity and colossal magnetoresistance.[1,2] However, high-quality RP film growth has been disturbed by extended defects, so-called out-of-phase boundaries (OPBs).[3] Since OPB formation hampers the functionalities of films, OPB suppression is highly required to carry out high-performance RP-based functional devices. [4]
Here, we suppressed OPBs in RP thin films using single-terminated LaSrAlO4 (LSAO) substrates. We developed a surface treatment recipe of LSAO substrates, which exhibited the uniform surface reconstruction having LaO-terminated surfaces. As a model system, the high-Tc cuprates La1.85Sr0.15CuO4 (LSCO) films were employed. On mixed-terminated LSAO surfaces, LSCO films exhibited huge OPB formations. In contrast, on single-terminated LSAO surfaces, the OPBs were suppressed. These OPB-free LSCO films exhibited significantly enhanced superconductivity (Tczero ~ 30 K) than the film with huge OPBs (Tczero ~ 5 K), under given thickness (~ 6.5 nm). By reflection high-energy electron diffraction (RHEED) and density functional theory (DFT) calculation, we observed that the LSCO stacking sequence can be controlled by LSAO surface termination.
Here, we suppressed OPBs in RP thin films using single-terminated LaSrAlO4 (LSAO) substrates. We developed a surface treatment recipe of LSAO substrates, which exhibited the uniform surface reconstruction having LaO-terminated surfaces. As a model system, the high-Tc cuprates La1.85Sr0.15CuO4 (LSCO) films were employed. On mixed-terminated LSAO surfaces, LSCO films exhibited huge OPB formations. In contrast, on single-terminated LSAO surfaces, the OPBs were suppressed. These OPB-free LSCO films exhibited significantly enhanced superconductivity (Tczero ~ 30 K) than the film with huge OPBs (Tczero ~ 5 K), under given thickness (~ 6.5 nm). By reflection high-energy electron diffraction (RHEED) and density functional theory (DFT) calculation, we observed that the LSCO stacking sequence can be controlled by LSAO surface termination.
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Publication: [1] J. G. Bednorz et al., Science 236 (1987) 73<br>[2] Y. Moritomo et al., Nature 380 (1996) 141<br>[3] M. A. Zurbuchen et al., J. Mater. Res., 22, 1439 (2007).<br>[4] J. Kim et al., Nano Lett. 21, 4185 (2021).
Presenters
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Jinkwon Kim
Seoul National University, Institute for Basic Science
Authors
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Jinkwon Kim
Seoul National University, Institute for Basic Science
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Youngdo Kim
Seoul National University, Seoul Natl Univ
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Junsik Mun
Seoul National University
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Tae Won Noh
Seoul National University, Seoul Natl Univ