Crystal growth, microstructure, and physical properties of SrMnSb2

Yong Liu, Tao Ma, Lin Zhou, Warren E. Straszheim, Farhan Islam, Brandt A. Jensen, Wei Tian, Thomas Heitmann, R. A. Rosenberg, J. M. Wilde, Bing Li, Andreas Kreyssig, Alan I. Goldman, B. G. Ueland, Robert J. McQueeney, and David Vaknin
Phys. Rev. B 99, 054435 – Published 28 February 2019

Abstract

We report on the crystal and magnetic structures and magnetic and transport properties of SrMnSb2 single crystals grown by the self-flux method. Magnetic susceptibility measurements reveal an antiferromagnetic (AFM) transition at TN=295(3) K. Above TN, the susceptibility slightly increases and forms a broad peak at T420 K, which is a typical feature of two-dimensional magnetic systems. Neutron diffraction measurements on single crystals confirm the previously reported C-type AFM structure below TN. Both de Haas-van Alphen (dHvA) and Shubnikov-de Haas (SdH) effects are observed in SrMnSb2 single crystals. Analysis of the oscillatory component by a Fourier transform shows that the prominent frequencies obtained by the two different techniques are practically the same within error regardless of sample size or saturated magnetic moment. Transmission electron microscopy (TEM) reveals the existence of stacking faults in the crystals, which result from a horizontal shift of Sb atomic layers suggesting possible ordering of Sb vacancies in the crystals. Increase of temperature in susceptibility measurements leads to the formation of a strong peak at T570 K that upon cooling under magnetic field the susceptibility shows a ferromagnetic transition at TC580 K. Neutron powder diffraction on crushed single crystals does not support a ferromagnetic phase above TN. Furthermore, x-ray magnetic circular dichroism (XMCD) measurements of a single crystal at the L2,3 edge of Mn shows a signal due to induced canting of AFM moments by the applied magnetic field. All evidence strongly suggests that a chemical transformation at the surface of single crystals occurs above 500 K concurrently producing a minute amount of ferromagnetic impurity phase.

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  • Received 12 September 2018

DOI:https://doi.org/10.1103/PhysRevB.99.054435

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Yong Liu1,*, Tao Ma1, Lin Zhou1, Warren E. Straszheim1, Farhan Islam1, Brandt A. Jensen1, Wei Tian2, Thomas Heitmann3, R. A. Rosenberg4, J. M. Wilde1,5, Bing Li1,5, Andreas Kreyssig1,5, Alan I. Goldman1,5, B. G. Ueland1,5, Robert J. McQueeney1,5, and David Vaknin1,5,†

  • 1Division of Materials Sciences and Engineering, Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA
  • 2Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3The Missouri Research Reactor, University of Missouri, Columbia, Missouri 65211, USA
  • 4Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 5Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA

  • *yongliu31@outlook.com
  • vaknin@ameslab.gov

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Issue

Vol. 99, Iss. 5 — 1 February 2019

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