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Ferromagnetic spin fluctuations in the filled skutterudite SrFe4As12 revealed by As75 NMR-NQR measurements

Q.-P. Ding, K. Rana, K. Nishine, Y. Kawamura, J. Hayashi, C. Sekine, and Y. Furukawa
Phys. Rev. B 98, 155149 – Published 31 October 2018

Abstract

As75 nuclear magnetic resonance (NMR) and nuclear quadrupole resonance (NQR) measurements have been carried out to investigate the magnetic and electronic properties of the filled skutterudite metallic compound SrFe4As12. The temperature dependence of Knight shift K determined by the NQR spectrum under a small magnetic field (0.5T) shows the similar temperature dependence of the magnetic susceptibility χ which exhibits a broad maximum at T*50 K. The nuclear spin-lattice relaxation rate divided by temperature 1/T1T increases with decreasing temperature and exhibits a broad maximum at T70 K, similar to the case of χ. The temperature dependence of K and 1/T1T is reasonably explained by a simple model where we assume a concave-shaped band structure near the Fermi energy. Based on a Korringa ratio analysis using the T1 and K data, ferromagnetic spin fluctuations are found to exist in SrFe4As12. These results indicate that SrFe4As12 can be characterized to be a metal with ferromagnetic correlations and also the peculiar band structure responsible for the suppression of 1/T1T and K at low temperatures.

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  • Received 18 August 2018
  • Revised 9 October 2018

DOI:https://doi.org/10.1103/PhysRevB.98.155149

©2018 American Physical Society

Physics Subject Headings (PhySH)

  1. Research Areas
  1. Physical Systems
Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Q.-P. Ding1, K. Rana1, K. Nishine2, Y. Kawamura2, J. Hayashi2, C. Sekine2, and Y. Furukawa1

  • 1Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
  • 2Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan

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Issue

Vol. 98, Iss. 15 — 15 October 2018

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Images

  • Figure 1
    Figure 1

    Field-swept AsNMR75 spectra of SrFe4As12 at f=37 MHz and T=4.3 K. Black curve is the observed spectrum and red curve is the calculated spectrum with νQ=54.8 MHz, η=0.4. Blue dotted curve represents the calculated As75 NMR spectrum (νQ=23.5 MHz, η=0) from the impurity phase [23]. The sum of the two calculated spectra is shown by the green area.

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  • Figure 2
    Figure 2

    (a) T dependence of the As75-NQR spectra for SrFe4As12. (b) T dependence of As75-NQR frequency νNQR in SrFe4As12. The inset shows the As75-NQR frequency νNQR vs T3/2 plot, indicating a monotonous decrease following T3/2 above 40 K.

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  • Figure 3
    Figure 3

    (a) Representative As75-NQR spectra under zero and 0.5 T magnetic field at 4.3 K. The blue curve is a simulated powder-pattern spectrum with νQ=54.8 MHz, η=0.4, and H=0.5 T. The arrow shows the position of the lower-frequency edge position (fL) whose position can be calculated from θ=π (and also θ=0). The inset shows the external magnetic field dependence of fL. (b) T dependence of As75 Knight shift K. The solid curves are the calculated results (see text). The inset shows K(T) versus magnetic susceptibility χ(T). The red dash line is a linear fit.

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  • Figure 4
    Figure 4

    Temperature dependencies of 1/T1T in SrFe4As12. The solid line is the calculated result based on the simple band structure shown in the lower inset with a set of parameters of Δ=88 K, W=220 K, and rD1/D0=0.38. The upper inset shows the frequency dependence of 1/T1T measured at T=4.3 K and H=0.5 T, together with the spectrum at the same condition. No obvious change in the frequency dependence of 1/T1T indicates that 1/T1 is nearly isotropic within the experimental uncertainty.

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  • Figure 5
    Figure 5

    T dependence of Korringa ratio K(α) in SrFe4As12.

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