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.
Original language | English |
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Article number | 3122 |
Journal | Nature Communications |
Volume | 12 |
Issue number | 1 |
DOIs | |
State | Published - Dec 1 2021 |
Funding
We acknowledge John Tranquada, Rafael Fernandes, Connor Occhialini, and Andrey Chubukov for enlightening discussions. We also thank Nick Brookes, Kurt Kummer, and Davide Betto for initial tests on FeSe/STO. This work was supported by the Air Force Office of Scientific Research Young Investigator Program under grant FA9550-19-1-0063 (J.P. and R.C.). We thank Diamond Light Source for the allocation of beamtime to proposal SP18883. J.P. acknowledges financial support by the Swiss National Science Foundation Early Postdoc Mobility Fellowship Project No. P2FRP2_171824 and P400P2_180744. S.K., T.A.M., and S.J. are supported by the Scientific Discovery through Advanced Computing (SciDAC) program funded by U.S. Department of Energy, Office of Science, Advanced Scientific Computing Research and Basic Energy Sciences, Division of Materials Sciences and Engineering. S.J. acknowledges additional support from the Office of Naval Research under Grant No. N00014-18-1-2675. An award of computer time was provided by the INCITE program. This research also used resources of the Oak Ridge Leadership Computing Facility, which is a DOE Office of Science User Facility supported under Contract DE-AC05-00OR22725. M.R. and G.G. were supported by the ERC-P-ReXS project (2016-0790) of the Fondazione CARIPLO and Regione Lombardia, in Italy. R.A. is supported by the Swedish Research Council (VR) under the Project 2017-00382. R.C. acknowledges support from the Alfred P. Sloan Foundation. X. C, R.P. and D.L.F acknowledge the support from National Natural Science Foundation of China (Nos. 11790310 and 11922403). R.C. and G.G. acknowledge support from the MIT-POLIMI Program (Progetto Rocca) of the MIT International Science and Technology Initiatives (MISTI) and Politecnico di Milano.
Funders | Funder number |
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MIT International Science and Technology Initiatives | |
MIT-POLIMI | |
Office of Naval Research | N00014-18-1-2675 |
U.S. Department of Energy | |
Air Force Office of Scientific Research | FA9550-19-1-0063 |
Alfred P. Sloan Foundation | |
Office of Science | DE-AC05-00OR22725, 2016-0790 |
Advanced Scientific Computing Research | |
U.S. Air Force | |
Division of Materials Sciences and Engineering | |
National Outstanding Youth Science Fund Project of National Natural Science Foundation of China | 11922403 |
Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung | P2FRP2_171824, P400P2_180744 |
National Natural Science Foundation of China | 11790310 |
Fondazione Cariplo | |
Vetenskapsrådet | 2017-00382 |
Politecnico di Milano | |
Regione Lombardia |