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Title: Hot-lines topology and the fate of the spin resonance mode in three-dimensional unconventional superconductors

Abstract

In the quasi-two-dimensional (quasi-2D) copper- and iron-based superconductors, the onset of superconductivity is accompanied by a prominent peak in the magnetic spectrum at momenta close to the wave-vector of the nearby antiferromagnetic state. Such a peak is well described in terms of a spin resonance mode, i.e., a spin-1 exciton theoretically predicted for quasi-2D superconductors with a sign-changing gap. The same theories, however, indicate that such a resonance mode should be absent in a three-dimensional (3D) system with a spherical Fermi surface. This raises the question of the fate of the spin resonance mode in layered unconventional superconductors that are not strongly anisotropic, such as certain heavy-fermion compounds and potentially the newly discovered nickelate superconductor NdNiO2. Here, we use the random phase approximation to calculate the dynamical spin susceptibility of 3D superconductors with a dx2–y2-wave gap symmetry and corrugated cylindrical-like Fermi surfaces. By varying the out-of-plane hopping anisotropy tz/t, we demonstrate that the appearance of a spin resonance mode is determined by the topology of the hot lines, i.e., lines on the Fermi surface that are connected by the magnetic wave vector. For an in-plane antiferromagnetic wave vector, the hot lines undergo a topological transition from open lines to closedmore » loops at a critical tz/t value. The closed hot lines cross the nodal superconducting lines, making the spin resonance mode overdamped and incoherent. In contrast, for an out-of-plane antiferromagnetic wave vector, the hot lines remain open and the spin resonance mode remains sharp. We discuss the experimental implications of our results for the out-of-plane dispersion of the spin resonance mode and, more generally, for inelastic neutron scattering experiments on unconventional superconductors.« less

Authors:
ORCiD logo [1];  [1]; ORCiD logo [2]
  1. Univ. of Minnesota, Minneapolis, MN (United States)
  2. Univ. of Copenhagen (Denmark). The Niels Bohr Inst.
Publication Date:
Research Org.:
Univ. of Minnesota, Minneapolis, MN (United States)
Sponsoring Org.:
USDOE Office of Science (SC)
OSTI Identifier:
1979788
Grant/Contract Number:  
SC0016371
Resource Type:
Accepted Manuscript
Journal Name:
Physical Review. B
Additional Journal Information:
Journal Volume: 106; Journal Issue: 1; Journal ID: ISSN 2469-9950
Publisher:
American Physical Society (APS)
Country of Publication:
United States
Language:
English
Subject:
36 MATERIALS SCIENCE; Physics; magnetic susceptibility; superconductivity; unconventional superconductors

Citation Formats

Chen, Fei, Fernandes, Rafael M., and Christensen, Morten H. Hot-lines topology and the fate of the spin resonance mode in three-dimensional unconventional superconductors. United States: N. p., 2022. Web. doi:10.1103/physrevb.106.014511.
Chen, Fei, Fernandes, Rafael M., & Christensen, Morten H. Hot-lines topology and the fate of the spin resonance mode in three-dimensional unconventional superconductors. United States. https://doi.org/10.1103/physrevb.106.014511
Chen, Fei, Fernandes, Rafael M., and Christensen, Morten H. Mon . "Hot-lines topology and the fate of the spin resonance mode in three-dimensional unconventional superconductors". United States. https://doi.org/10.1103/physrevb.106.014511. https://www.osti.gov/servlets/purl/1979788.
@article{osti_1979788,
title = {Hot-lines topology and the fate of the spin resonance mode in three-dimensional unconventional superconductors},
author = {Chen, Fei and Fernandes, Rafael M. and Christensen, Morten H.},
abstractNote = {In the quasi-two-dimensional (quasi-2D) copper- and iron-based superconductors, the onset of superconductivity is accompanied by a prominent peak in the magnetic spectrum at momenta close to the wave-vector of the nearby antiferromagnetic state. Such a peak is well described in terms of a spin resonance mode, i.e., a spin-1 exciton theoretically predicted for quasi-2D superconductors with a sign-changing gap. The same theories, however, indicate that such a resonance mode should be absent in a three-dimensional (3D) system with a spherical Fermi surface. This raises the question of the fate of the spin resonance mode in layered unconventional superconductors that are not strongly anisotropic, such as certain heavy-fermion compounds and potentially the newly discovered nickelate superconductor NdNiO2. Here, we use the random phase approximation to calculate the dynamical spin susceptibility of 3D superconductors with a dx2–y2-wave gap symmetry and corrugated cylindrical-like Fermi surfaces. By varying the out-of-plane hopping anisotropy tz/t, we demonstrate that the appearance of a spin resonance mode is determined by the topology of the hot lines, i.e., lines on the Fermi surface that are connected by the magnetic wave vector. For an in-plane antiferromagnetic wave vector, the hot lines undergo a topological transition from open lines to closed loops at a critical tz/t value. The closed hot lines cross the nodal superconducting lines, making the spin resonance mode overdamped and incoherent. In contrast, for an out-of-plane antiferromagnetic wave vector, the hot lines remain open and the spin resonance mode remains sharp. We discuss the experimental implications of our results for the out-of-plane dispersion of the spin resonance mode and, more generally, for inelastic neutron scattering experiments on unconventional superconductors.},
doi = {10.1103/physrevb.106.014511},
journal = {Physical Review. B},
number = 1,
volume = 106,
place = {United States},
year = {Mon Jul 18 00:00:00 EDT 2022},
month = {Mon Jul 18 00:00:00 EDT 2022}
}

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