Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe

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Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe. / Steffensen, Daniel; Kreisel, Andreas; Hirschfeld, P. J.; Andersen, Brian M.

In: Physical Review B, Vol. 103, No. 5, 054505, 15.02.2021.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Steffensen, D, Kreisel, A, Hirschfeld, PJ & Andersen, BM 2021, 'Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe', Physical Review B, vol. 103, no. 5, 054505. https://doi.org/10.1103/PhysRevB.103.054505

APA

Steffensen, D., Kreisel, A., Hirschfeld, P. J., & Andersen, B. M. (2021). Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe. Physical Review B, 103(5), [054505]. https://doi.org/10.1103/PhysRevB.103.054505

Vancouver

Steffensen D, Kreisel A, Hirschfeld PJ, Andersen BM. Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe. Physical Review B. 2021 Feb 15;103(5). 054505. https://doi.org/10.1103/PhysRevB.103.054505

Author

Steffensen, Daniel ; Kreisel, Andreas ; Hirschfeld, P. J. ; Andersen, Brian M. / Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe. In: Physical Review B. 2021 ; Vol. 103, No. 5.

Bibtex

@article{ae078bb570a64c998dbf210529059106,
title = "Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe",
abstract = "The electronic structure of the enigmatic iron-based superconductor FeSe has puzzled researchers since spectroscopic probes failed to observe the expected electron pocket at the Y point in the 1-Fe Brillouin zone. It has been speculated that this pocket, essential for an understanding of the superconducting state, is either absent or incoherent. Here, we perform a theoretical study of the preferred nematic order originating from nearest-neighbor Coulomb interactions in an electronic model relevant for FeSe. We find that at low temperatures the dominating nematic components are of interorbital d(xz)-d(xy) and d(yz)-d(xy) character, with spontaneously broken amplitudes for these two components. This interorbital nematic order naturally leads to distinct hybridization gaps at the X and Y points of the 1-Fe Brillouin zone, and may thereby produce highly anisotropic Fermi surfaces with only a single electron pocket at one of these momentum-space locations. The associated superconducting gap structure obtained with the generated low-energy electronic band structure from spin-fluctuation mediated pairing agrees well with that measured experimentally. Finally, from a comparison of the computed spin susceptibility to available neutron scattering data, we discuss the necessity of additional self-energy effects, and explore the role of orbital-dependent quasiparticle weights as a minimal means to include them.",
author = "Daniel Steffensen and Andreas Kreisel and Hirschfeld, {P. J.} and Andersen, {Brian M.}",
year = "2021",
month = feb,
day = "15",
doi = "10.1103/PhysRevB.103.054505",
language = "English",
volume = "103",
journal = "Physical Review B",
issn = "2469-9950",
publisher = "American Physical Society",
number = "5",

}

RIS

TY - JOUR

T1 - Interorbital nematicity and the origin of a single electron Fermi pocket in FeSe

AU - Steffensen, Daniel

AU - Kreisel, Andreas

AU - Hirschfeld, P. J.

AU - Andersen, Brian M.

PY - 2021/2/15

Y1 - 2021/2/15

N2 - The electronic structure of the enigmatic iron-based superconductor FeSe has puzzled researchers since spectroscopic probes failed to observe the expected electron pocket at the Y point in the 1-Fe Brillouin zone. It has been speculated that this pocket, essential for an understanding of the superconducting state, is either absent or incoherent. Here, we perform a theoretical study of the preferred nematic order originating from nearest-neighbor Coulomb interactions in an electronic model relevant for FeSe. We find that at low temperatures the dominating nematic components are of interorbital d(xz)-d(xy) and d(yz)-d(xy) character, with spontaneously broken amplitudes for these two components. This interorbital nematic order naturally leads to distinct hybridization gaps at the X and Y points of the 1-Fe Brillouin zone, and may thereby produce highly anisotropic Fermi surfaces with only a single electron pocket at one of these momentum-space locations. The associated superconducting gap structure obtained with the generated low-energy electronic band structure from spin-fluctuation mediated pairing agrees well with that measured experimentally. Finally, from a comparison of the computed spin susceptibility to available neutron scattering data, we discuss the necessity of additional self-energy effects, and explore the role of orbital-dependent quasiparticle weights as a minimal means to include them.

AB - The electronic structure of the enigmatic iron-based superconductor FeSe has puzzled researchers since spectroscopic probes failed to observe the expected electron pocket at the Y point in the 1-Fe Brillouin zone. It has been speculated that this pocket, essential for an understanding of the superconducting state, is either absent or incoherent. Here, we perform a theoretical study of the preferred nematic order originating from nearest-neighbor Coulomb interactions in an electronic model relevant for FeSe. We find that at low temperatures the dominating nematic components are of interorbital d(xz)-d(xy) and d(yz)-d(xy) character, with spontaneously broken amplitudes for these two components. This interorbital nematic order naturally leads to distinct hybridization gaps at the X and Y points of the 1-Fe Brillouin zone, and may thereby produce highly anisotropic Fermi surfaces with only a single electron pocket at one of these momentum-space locations. The associated superconducting gap structure obtained with the generated low-energy electronic band structure from spin-fluctuation mediated pairing agrees well with that measured experimentally. Finally, from a comparison of the computed spin susceptibility to available neutron scattering data, we discuss the necessity of additional self-energy effects, and explore the role of orbital-dependent quasiparticle weights as a minimal means to include them.

U2 - 10.1103/PhysRevB.103.054505

DO - 10.1103/PhysRevB.103.054505

M3 - Journal article

VL - 103

JO - Physical Review B

JF - Physical Review B

SN - 2469-9950

IS - 5

M1 - 054505

ER -

ID: 258400233