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Title: Structure of spin excitations in heavily electron-doped Li0.8Fe0.2ODFeSe superconductors

Journal Article · · Nature Communications
 [1]; ORCiD logo [1];  [1];  [1]; ORCiD logo [2]; ORCiD logo [3];  [1];  [1];  [1];  [4];  [5]; ORCiD logo [6]
  1. Fudan Univ., Shanghai (China). State Key Laboratory of Surface Physics and Department of Physics
  2. Technical University of Munich (Germany). Heinz Maier-Leibnitz Zentrum (MLZ)
  3. Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States).Quantum Condensed Matter Division; Univ. of Tennessee, Knoxville, TN (United States). Dept. of Physics and Astronomy
  4. Beijing Normal University (China). Department of Physics and Center for Advanced Quantum Studies
  5. Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States). Computer Science and Mathematics Division, Center for Nanophase Materials Sciences, and Materials Science and Technology Division
  6. Fudan Univ., Shanghai (China). State Key Laboratory of Surface Physics and Department of Physics; Collaborative Innovation Center of Advanced Microstructures, Nanjing (China)

Heavily electron-doped iron-selenide high-transition-temperature (high-Tc) superconductors, which have no hole Fermi pockets, but have a notably high Tc, have challenged the prevailing s± pairing scenario originally proposed for iron pnictides containing both electron and hole pockets. The microscopic mechanism underlying the enhanced superconductivity in heavily electron-doped iron-selenide remains unclear. Here, we used neutron scattering to study the spin excitations of the heavily electron-doped iron-selenide material Li0.8Fe0.2ODFeSe (Tc = 41 K). Our data revealed nearly ring-shaped magnetic resonant excitations surrounding (π, π) at ~21 meV. As the energy increased, the spin excitations assumed a diamond shape, and they dispersed outward until the energy reached ~60 meV and then inward at higher energies. The observed energy-dependent momentum structure and twisted dispersion of spin excitations near (π, π) are analogous to those of hole-doped cuprates in several aspects, thus implying that such spin excitations are essential for the remarkably high Tc in these materials.

Research Organization:
Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Basic Energy Sciences (BES) (SC-22). Materials Sciences & Engineering Division
Grant/Contract Number:
AC05-00OR22725
OSTI ID:
1399978
Journal Information:
Nature Communications, Vol. 8, Issue 1; ISSN 2041-1723
Publisher:
Nature Publishing GroupCopyright Statement
Country of Publication:
United States
Language:
English
Citation Metrics:
Cited by: 31 works
Citation information provided by
Web of Science

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Cited By (6)

Sign reversal of the order parameter in (Li1−xFex)OHFe1−yZnySe journal October 2017
Fermi surface pockets in electron-doped iron superconductor by Lifshitz transition journal October 2018
Coexistence of Ferromagnetic and Stripe-Type Antiferromagnetic Spin Fluctuations in YFe 2 Ge 2 journal May 2019
Neutron Spin Resonance in the Heavily Hole-Doped KFe 2 As 2 Superconductor journal January 2020
Nematicity and superconductivity in orthorhombic superconductor N a 0.35 ( C 3 N 2 H 10 ) 0.426 F e 2 S e 2 journal November 2018
Fermi surface pockets in electron-doped iron superconductor by Lifshitz transition text January 2018

Figures / Tables (5)