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Abstract
Spin degree of freedom generally plays an important role in unconventional superconductivity. In many of the iron-based compounds, superconductivity is found in close proximity to long-range antiferromagnetic order, whereas monolayer FeSe grown on SrTiO3, with enhanced superconductivity, exhibits no magnetic or nematic ordering. Here we grow monolayer and multilayer FeSe on antiferromagnetic EuTiO3(001) layers, in an effort to introduce a spin polarization in proximity to the superconductivity of FeSe. By X-ray magnetic dichroism, we observe an antiferromagnet–ferromagnet switching on Eu and Ti sites in EuTiO3 driven by the applied magnetic field, with no concomitant spin polarization on the Fe site of FeSe. Transport measurements show enhanced superconductivity of monolayer FeSe on EuTiO3 with a transition temperature of ~30 K. The band structure revealed by photoemission spectroscopy is analogous to that of FeSe/SrTiO3. Our work creates a platform for the interplay of spin and unconventional superconductivity in the two-dimensional limit.
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1 University of British Columbia, Quantum Matter Institute, Vancouver, Canada (GRID:grid.17091.3e) (ISNI:0000 0001 2288 9830); University of British Columbia, Department of Physics and Astronomy, Vancouver, Canada (GRID:grid.17091.3e) (ISNI:0000 0001 2288 9830)
2 Swiss Light Source, Paul Scherrer Institut, Villigen PSI, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
3 University of British Columbia, Quantum Matter Institute, Vancouver, Canada (GRID:grid.17091.3e) (ISNI:0000 0001 2288 9830); University of British Columbia, Department of Physics and Astronomy, Vancouver, Canada (GRID:grid.17091.3e) (ISNI:0000 0001 2288 9830); Max Planck Institute for Chemical Physics of Solids, Dresden, Germany (GRID:grid.419507.e) (ISNI:0000 0004 0491 351X)