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Suppression of ferromagnetic spin fluctuations in the filled skutterudite superconductor SrOs4As12 revealed by As75 NMR-NQR measurements

Q.-P. Ding, K. Nishine, Y. Kawamura, J. Hayashi, C. Sekine, and Y. Furukawa
Phys. Rev. B 100, 054516 – Published 26 August 2019

Abstract

Motivated by the recent observation of ferromagnetic spin correlations in the filled skutterudite SrFe4As12 [Q.-P. Ding et al., Phys. Rev. B 98, 155149 (2018)], we have carried out As75 nuclear magnetic resonance (NMR) and nuclear quadrupole resonance (NQR) measurements to investigate the role of magnetic fluctuations in the newly discovered isostructural superconductor SrOs4As12 with a superconducting transition temperature of Tc4.8K. Knight shift K determined by the NQR spectrum under a small magnetic field (0.5 T) is nearly independent of temperature, consistent with the temperature dependence of the magnetic susceptibility. The nuclear spin-lattice relaxation rate divided by temperature, 1/T1T, is nearly independent of temperature above 50 K and increases slightly with decreasing temperature below the temperature. The temperature dependence is reasonably explained by a simple model where a flat band structure with a small ledge near the Fermi energy is assumed. By comparing the present NMR data with those in SrFe4As12, we found that the values of |K| and 1/T1T in SrOs4As12 are smaller than those in SrFe4As12, indicating no obvious ferromagnetic spin correlations in SrOs4As12. From the temperature dependence of 1/T1 in the superconducting state, an s-wave superconductivity is realized.

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  • Received 23 May 2019
  • Revised 22 July 2019

DOI:https://doi.org/10.1103/PhysRevB.100.054516

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Q.-P. Ding1, 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. 100, Iss. 5 — 1 August 2019

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Images

  • Figure 1
    Figure 1

    Field-swept As75 NMR spectra of SrOs4As12 at f=37MHz and T=4.3K. The black curve is the observed spectrum, and the red curve is the calculated spectrum with νQ=60.1MHz, η=0.45. The blue dashed curve represents the calculated As75 NMR spectrum (νQ=23.5MHz, η=0) from the impurity phase [33]. The sum of the two calculated spectra is shown by the green area.

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  • Figure 2
    Figure 2

    (a) As75 NQR spectra measured at T=10K under zero magnetic field (top panel) and 0.5 T (bottom panel) in SrOs4As12. The red curve in the bottom panel is a simulated powder-pattern spectrum with νQ=60.1MHz, η=0.45, and H=0.5T. The arrow shows the position of the lower-frequency edge position fL, whose position is attributed to θ=π (and also θ=0). (b) T dependence of As75 NQR frequency νNQR in SrOs4As12. The black curve is νNQR(T)=νNQR(0)(1αQT3/2), with αQ=2.09×106K3/2 and νNQR(0)=62.14MHz. (c) The external magnetic field dependence of fL at T=10K.

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  • Figure 3
    Figure 3

    Temperature dependence of the As75 Knight shift K in SrOs4As12 (red circles) and SrFe4As12 (black squares) from Ref. [33]. Temperature dependences of the magnetic susceptibility χ are also plotted by the red and black curves for SrOs4As12 and SrFe4As12 [31], respectively. The inset shows K versus the corresponding magnetic susceptibility χ. The black line is a linear fit.

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  • Figure 4
    Figure 4

    Temperature dependences of As75 1/T1T in SrOs4As12 (red circles) and SrFe4As12 (black squares) from Ref. [33]. The solid lines are the calculated results based on the band structures near EF shown in the inset with the following set of parameters: ΔOs=40K and D0,Os/D1,Os=1.2 for SrOs4As12 and ΔFe=88K, W=220K, and D0,Fe/D1,Fe=2.6 for SrFe4As12.

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  • Figure 5
    Figure 5

    (a) Temperature dependence of 1/T1 in SrOs4As12. The pink curve in the superconducting state is the calculated result based on the BCS theory The red curve in the normal state is the calculated results shown in Fig. 4. The inset shows the temperature dependence of β. (b) Temperature dependence of electrical resistivity from Ref. [31]. (c) Temperature dependence of volume magnetic susceptibility in the superconducting state estimated from the zero-field-cooled magnetic susceptibility data reported in Ref. [31]. (d) Temperature dependence of 1/T1T in the low-temperature region together with the calculated result (pink curve) based on BCS theory. The vertical blue lines are just guides to the eye.

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