Granular superconductivity and charge/orbital order in YBa 2 Cu 3 O 7 /manganite trilayers
Khmaladze, JarjiDepartment of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Switzerland
Sarkar, SubhrangsuDepartment of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Switzerland
Soulier, MathiasDepartment of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Switzerland
Lyzwa, FryderykDepartment of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Switzerland
Prada, R. de AndresDepartment of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Switzerland
Perret, EdithDepartment of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Switzerland - Laboratory for Advanced Fibers, Empa, Swiss Federal Laboratories for Materials Science and Technology, St. Gallen, Switzerland
Mallett, Benjamin P. P.The MacDiarmid Institute and the Dodd Walls Centre for Photonic and Quantum Technologies, Photon Factory, University of Auckland, New Zealand
Minola, M.Max-Planck-Institut für Festkörperforschung, Stuttgart, Germany
Keimer, B.Max-Planck-Institut für Festkörperforschung, Stuttgart, Germany
Bernhard, ChristianDepartment of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Switzerland
English
We studied how the electronic, superconducting, and magnetic properties of YBa2Cu3O7/Nd1−x(Ca1−ySry )xMnO3 multilayers depend on the tolerance factor and the hole doping of the manganite. In particular, we investigated the granular superconducting state and the related magnetic-field-driven insulator-to- superconductor transition that was previously discovered in corresponding multilayers with Pr0.5La0.2Ca0.3MnO3 [B. P. P. Mallett et al., Phys. Rev. B 94, 180503(R) (2016)]. We found that this granular uperconducting state occurs only when the manganite layer is in a charge/orbital ordered and CE-type antiferromagnetic state (Mn-CO/OO). The coupling mechanism underlying this intriguing proximity effect seems to involve the domain boundaries of the Mn-CO/OO and/or the charge disordered regions of the manganite layer that become more numerous as the hole doping is reduced below x = 0.5.