Magnetic field-induced abrupt enhancement in critical current density in LSMO/YBCO/LSMO/STO heterostructures
ORAL
Abstract
In this study, we report the influence of the complex coupling at the high-Tc-superconductor/oxide-ferromagnetic interface of LSMO/YBCO/LSMO trilayer heterostructures in terms of the superconducting critical current (Ic). We grew epitaxial tri-layer thin films by using the PLD technique, where LSMO bottom and top layer thicknesses were 10 nm and 15 nm, respectively, while the thickness of the middle YBCO layer was 15nm and 30 nm for the LY15L and the LY30L heterostructure respectively. In order to study the interface effect, the initial interface conditions (the work function difference, the orbital hybridization, and the magnetic coupling between the induced Cu and Mn moments) were preset by a cooling process with various field-cooled fields (FCF). In the FCF process, the sample was cooled down from 120K to 40K under a magnetic field parallel to the film surface and along the direction of the applied in-plane current. The Ic as a function of the FCF shows that Ic initially increases at lower FCF and attains maximum Ic at the intermediate range and then it starts to decrease with further increase in FCF. We observed the critical current Ic was greatly enhanced by ~18% at 0.5T for the LY15L and ~90% at 0.6T for the LY30L heterostructures. Moreover, we also observed the Ic increases with the increase in the applied magnetic field (AF) for the LY15L heterostructure. This behavior is opposite to a normal superconducting system where Ic decreases with the increase in the applied magnetic field, and strongly implies the possible existence of triplet superconducting pairs at the interface and inside the FM layer. We proposed phenomenological and combination models which are based on singlet and triplet superconductivity mechanisms to explain the enhancement in critical current at the interface of LSMO/YBCO/LSMO heterostructures.
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Presenters
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Sagar Mal M Kumawat
Department of Physics and Center of Crystal Research, National Sun Yat-sen University, Kaohsiung, Taiwan, 80424, R.O.C, Department of Physics, and Center of Crystal Research, National Sun Yat-sen University, Kaohsiung, 80424, Taiwan, National Sun Yat-sen University
Authors
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Sagar Mal M Kumawat
Department of Physics and Center of Crystal Research, National Sun Yat-sen University, Kaohsiung, Taiwan, 80424, R.O.C, Department of Physics, and Center of Crystal Research, National Sun Yat-sen University, Kaohsiung, 80424, Taiwan, National Sun Yat-sen University