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Abstract
In ultrathin films of FeSe grown on SrTiO3 (FeSe/STO), the superconducting transition temperature Tc is increased by almost an order of magnitude, raising questions on the pairing mechanism. As in other superconductors, antiferromagnetic spin fluctuations have been proposed to mediate SC making it essential to study the evolution of the spin dynamics of FeSe from the bulk to the ultrathin limit. Here, we investigate the spin excitations in bulk and monolayer FeSe/STO using resonant inelastic x-ray scattering (RIXS) and quantum Monte Carlo (QMC) calculations. Despite the absence of long-range magnetic order, bulk FeSe displays dispersive magnetic excitations reminiscent of other Fe-pnictides. Conversely, the spin excitations in FeSe/STO are gapped, dispersionless, and significantly hardened relative to its bulk counterpart. By comparing our RIXS results with simulations of a bilayer Hubbard model, we connect the evolution of the spin excitations to the Fermiology of the two systems revealing a remarkable reconfiguration of spin excitations in FeSe/STO, essential to understand the role of spin fluctuations in the pairing mechanism.
Here, Pelliciari et al. present resonant inelastic X-ray scattering on monolayer samples of unconventional superconductor FeSe, finding evidence for gapped and dispersionless spin excitations. These experiments are very difficult due to the extremely small scattering volume of the FeSe monolayer.
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1 Massachusetts Institute of Technology, Department of Physics, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786); NSLS-II, Brookhaven National Laboratory, Upton, USA (GRID:grid.202665.5) (ISNI:0000 0001 2188 4229)
2 Oak Ridge National Laboratory, Center for Nanophase Materials Sciences, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)
3 Fudan University, State Key laboratory of Surface Physics and Department of Physics, Shanghai, China (GRID:grid.8547.e) (ISNI:0000 0001 0125 2443)
4 Politecnico di Milano, Dipartimento di Fisica, Milano, Italy (GRID:grid.4643.5) (ISNI:0000 0004 1937 0327); Chalmers University of Technology, Quantum Device Physics Laboratory, Department of Microtechnology and Nanoscience, Göteborg, Sweden (GRID:grid.5371.0) (ISNI:0000 0001 0775 6028)
5 Diamond Light Source, Didcot, UK (GRID:grid.18785.33) (ISNI:0000 0004 1764 0696)
6 Politecnico di Milano, Dipartimento di Fisica, Milano, Italy (GRID:grid.4643.5) (ISNI:0000 0004 1937 0327)
7 Politecnico di Milano, Dipartimento di Fisica, Milano, Italy (GRID:grid.4643.5) (ISNI:0000 0004 1937 0327); Politecnico di Milano, CNR-SPIN, Dipartimento di Fisica, Milano, Italy (GRID:grid.4643.5) (ISNI:0000 0004 1937 0327)
8 Oak Ridge National Laboratory, Center for Nanophase Materials Sciences, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659); Oak Ridge National Laboratory, Computational Sciences and Engineering Division, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)
9 The University of Tennessee, Department of Physics and Astronomy, Knoxville, USA (GRID:grid.411461.7) (ISNI:0000 0001 2315 1184)
10 Massachusetts Institute of Technology, Department of Physics, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)