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Muon spin rotation study of the topological superconductor SrxBi2Se3

H. Leng, D. Cherian, Y. K. Huang, J.-C. Orain, A. Amato, and A. de Visser
Phys. Rev. B 97, 054503 – Published 5 February 2018
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Abstract

We report transverse-field (TF) muon spin rotation experiments on single crystals of the topological superconductor SrxBi2Se3 with nominal concentrations x=0.15 and 0.18 (Tc3 K). The TF spectra (B=10 mT), measured after cooling to below Tc in field, did not show any additional damping of the muon precession signal due to the flux line lattice within the experimental uncertainty. This puts a lower bound on the magnetic penetration depth λ2.3μm. However, when we induce disorder in the vortex lattice by changing the magnetic field below Tc, a sizable damping rate is obtained for T0. The data provide microscopic evidence for a superconducting volume fraction of 70% in the x=0.18 crystal and thus bulk superconductivity.

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  • Received 20 September 2017

DOI:https://doi.org/10.1103/PhysRevB.97.054503

©2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

H. Leng1,*, D. Cherian1, Y. K. Huang1, J.-C. Orain2, A. Amato2, and A. de Visser1,†

  • 1Van der Waals–Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands
  • 2Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland

  • *h.leng@uva.nl
  • a.devisser@uva.nl

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Issue

Vol. 97, Iss. 5 — 1 February 2018

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Images

  • Figure 1
    Figure 1

    μSR spectra for Sr0.15Bi2Se3 measured in a transverse field of 10 mT (Ba) at T=3.0 K (upper panel) and T=0.25 K (lower panel). The red lines are fits using the muon depolarization function Eq. (1). The spectra are taken after field cooling in 10 mT.

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  • Figure 2
    Figure 2

    Temperature variation of the Gaussian damping rate σTF extracted with help of Eq. (1) from TF μSR spectra taken after field cooling in 10 mT. Green symbols: for x=0.15 and Ba. Blue symbols: for x=0.15 and Bc. Red symbols: for x=0.18 and Ba. The dashed horizontal lines show σTF is temperature-independent.

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  • Figure 3
    Figure 3

    μSR spectra for Sr0.18Bi2Se3 measured in a transverse field of 10 mT at T=3.0 K (upper panel) and T=0.25 K (lower panel). The crystal was cooled in a strong field of 0.4 T (Bc), after which the field was reduced to 10 mT. The red lines are fits to the muon depolarization function Eq. (4). The green and magenta lines in the lower panel represent the contributions to the μSR signal from the superconducting and normal state volume fractions, respectively.

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  • Figure 4
    Figure 4

    Fit parameters of the two-component analysis [Eq. (4)] of TF μSR spectra for Sr0.18Bi2Se3. Disorder in the vortex lattice is induced by changing the field below Tc. (a) σSC(T) (round symbols) and σN(T) (triangles). Green symbols: field-cooling in 0.4 T, spectra measured after reducing the field to TF=10 mT (Bc). Magenta symbols: cooling in 10 mT, spectra measured after sweeping the field first to zero and then up to TF=14.5 mT (Ba). (b) Superconducting fSC and normal-state fN volume fraction for cooling in 0.4 T (closed symbols) and 10 mT (open symbols). (c) ac susceptibility in SI units. The superconducting screening fraction is 0.7.

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