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Magnetic detwinning and biquadratic magnetic interaction in EuFe2As2 revealed by Eu153 NMR

Q.-P. Ding, N. S. Sangeetha, W. R. Meier, M. Xu, S. L. Bud'ko, P. C. Canfield, D. C. Johnston, and Y. Furukawa
Phys. Rev. B 102, 180406(R) – Published 10 November 2020
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Abstract

In the nematic state of iron-based superconductors, twin formation often obscures the intrinsic, anisotropic, in-plane physical properties. Relatively high in-plane external magnetic fields Hext greater than the typical laboratory-scale magnetic fields 10–15 T are usually required to completely detwin a sample. However, recently a very small in-plane Hext0.1 T was found to be sufficient for detwinning the nematic domains in EuFe2As2. To explain this behavior, a microscopic theory based on biquadratic magnetic interactions between the Eu and Fe spins has been proposed. Here, using Eu153 nuclear magnetic resonance (NMR) measurements below the Eu2+ ordering temperature, we show experimental evidence of the detwinning under small in-plane Hext. Our NMR study also reveals the evolution of the angles between the Eu and Fe spins during the detwinning process, which provides experimental evidence for the existence of biquadratic coupling in the system.

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  • Received 19 September 2020
  • Accepted 2 November 2020

DOI:https://doi.org/10.1103/PhysRevB.102.180406

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Q.-P. Ding, N. S. Sangeetha, W. R. Meier, M. Xu, S. L. Bud'ko, P. C. Canfield, D. C. Johnston, and Y. Furukawa

  • Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA

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Issue

Vol. 102, Iss. 18 — 1 November 2020

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Images

  • Figure 1
    Figure 1

    Eu153 NMR spectrum for Hext=0 at 4.3 K. The red lines are the calculated Eu153 NMR spectrum. The right figure shows the spin structure of EuFe2As2 in the orthorhombic phase under zero Hext.

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  • Figure 2
    Figure 2

    (a) Hext dependence of the Eu153 NMR spectra of EuFe2As2 for Hextc at T=4.3K. The red lines are calculated spectra with different values of θ and Heff under different Hext without changing other parameters: BintEu=27.0 T, νQ=40.2MHz, η=0.25, and ϕ=90. (b) Schematic view of the configuration for θ and the canting angles of θ and Θ between the magnetization and the quantization axis of Eu nucleus, respectively, from the ab plane in Hextc. (c) Hextc dependence of the angles θ, θ, and Θ estimated from the magnetization data at T=5K [27] and θ estimated from Eu153 NMR spectrum measurements.

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  • Figure 3
    Figure 3

    (a) Hext dependence of the Eu153 NMR spectrum for Hext[110]T at T=4.3K. The calculated positions of the spectra for the b and a domains are shown by the arrows in magenta and blue, respectively. The insets show a sketch of the spin directions of Eu (green) and Fe (brown) for the a (blue) and b (magenta) domains. (b) Hext dependence of the central peak of the Eu153 NMR spectrum for Hext[110]T. The inset shows a schematic view of the configuration for the angles ϕ, ϕ, and Φ in the ab plane for the case of Hextb. (c) Hext dependence of f of the central transition line for an a domain (blue) and a b domain (magenta). The solid lines are linear fits by f=ν0±αHeff with α=4MHz/T. (d) Hext dependence of domain population. (e) Hext dependence of the angle ϕH between Hext and the Eu spins for the a and b domains.

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