Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                

Frustrated magnetism in the tetragonal CoSe analog of superconducting FeSe

Brandon Wilfong, Xiuquan Zhou, Hector Vivanco, Daniel J. Campbell, Kefeng Wang, Dave Graf, Johnpierre Paglione, and Efrain Rodriguez
Phys. Rev. B 97, 104408 – Published 8 March 2018
PDFHTMLExport Citation

Abstract

Recently synthesized metastable tetragonal CoSe, isostructural to the FeSe superconductor, offers a new avenue for investigating systems in close proximity to the iron-based superconductors. We present magnetic and transport property measurements on powders and single crystals of CoSe. High field magnetic susceptibility measurements indicate a suppression of the previously reported 10 K ferromagnetic transition with the magnetic susceptibility, exhibiting time dependence below the proposed transition. Dynamic scaling analysis of the time dependence yields a critical relaxation time of τ*=0.064±0.008 s which in turn yields activation energy Ea*=14.84±0.59 K and an ideal glass temperature T0*=8.91±0.09 K from Vogel-Fulcher analysis. No transition is observed in resistivity and specific heat measurements, but both measurements indicate that CoSe is metallic. These results are interpreted on the basis of CoSe exhibiting frustrated magnetic ordering arising from competing magnetic interactions. Arrott analysis of single crystal magnetic susceptibility has indicated the transition temperature occurs in close proximity to previous reports and that the magnetic moment lies solely in the ab plane. The results have implications for understanding the relationship between magnetism and transport properties in the iron chalcogenide superconductors.

  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
  • Figure
  • Received 15 November 2017

DOI:https://doi.org/10.1103/PhysRevB.97.104408

©2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Brandon Wilfong1,2, Xiuquan Zhou1, Hector Vivanco1, Daniel J. Campbell2,3, Kefeng Wang2,3, Dave Graf4, Johnpierre Paglione2,3, and Efrain Rodriguez1,2,*

  • 1Department of Chemistry and Biochemistry, University of Maryland, College Park, Maryland 20742, USA
  • 2Center for Nanophysics and Advanced Materials, University of Maryland, College Park, Maryland 20742, USA
  • 3Department of Physics, University of Maryland, College Park, Maryland 20742, USA
  • 4National High Magnetic Field Laboratory, 1800 East Paul Dirac Drive, Tallahassee, Florida 32310, USA

  • *efrain@umd.edu

Article Text (Subscription Required)

Click to Expand

Supplemental Material (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 97, Iss. 10 — 1 March 2018

Reuse & Permissions
Access Options
CHORUS

Article Available via CHORUS

Download Accepted Manuscript
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1

    Crystal structures of KCo2Se2 and CoSe.

    Reuse & Permissions
  • Figure 2
    Figure 2

    Inverse magnetic susceptibility of CoSe vs temperature measured in an applied field of 100 Oe. The inverse magnetic susceptibility is fit from 100 to 300 K to the Curie-Weiss law plus a temperature-independent term. The inset shows inverse magnetic susceptibilities for different applied dc fields (0.2, 1, and 5 T) to emphasize the change in slope near 82 K.

    Reuse & Permissions
  • Figure 3
    Figure 3

    Magnetic susceptibility of CoSe vs temperature measured in various applied fields. The insets show the zoomed region close to the transition temperature; ZFC (zero-field-cooled) and FC (field-cooled) curves are shown by arrows which indicate the irreversibility of the magnetic ordering in the system at low fields. The bifurcation of ZFC-FC curves at low applied field (a) = 0.01 T and (b) = 0.2 T is destroyed with high applied fields (c) = 1 T and (d) = 5 T turning the system into a paramagnetic state with no irreversibility.

    Reuse & Permissions
  • Figure 4
    Figure 4

    Ac magnetic susceptibility measured with various driving frequencies. The applied ac field was 10 Oe and the residual dc applied field due to internal instrumentation was 40 to 100 Oe. (a) The real parts of magnetic susceptibility (χ) and (b) the imaginary parts (χ) parts. (c) Temperature dependence of χ peaks at various driving frequencies (100 to 1200 Hz) and a fit with the Volger-Fulcher law.

    Reuse & Permissions
  • Figure 5
    Figure 5

    Electrical transport measurements of CoSe single crystals obtained through de-intercalation of KCo2Se2. (a) Temperature dependence of longitudinal resistivity at various applied fields with the inset around the transition temperature. (b) Normalized longitudinal magnetoresistance up to 31 T with different applied field directions by sample rotation. (c) Angular dependence of longitudinal magnetoresistance at an applied field of 31 T. The magnetoresistance is fit with a sinusoidal dependence to the field angle.

    Reuse & Permissions
  • Figure 6
    Figure 6

    Temperature-dependent specific heat of a pressed pellet of CoSe from 150 K to base temperature. Upper inset shows the temperature dependence near the transition temperature as well as a fit to a specific heat model accounting for electronic and vibrational components in the range 1.8 to 15 K.

    Reuse & Permissions
  • Figure 7
    Figure 7

    Magnetic measurements of CoSe crystals mounted on a quartz paddle with orientations relative to the applied field direction as listed. (a) Temperature-dependent magnetic susceptibility for a 100 Oe field applied in two different orientations. (b) Field-dependent magnetization for both field orientations. (c) Arrott plots constructed from M(H) curves from 2 to 12 K for Hab, which indicate a ferromagnetic transiton within the 8–10 K range. (d) Arrott plots constructed for Hc axis showing no spontaneous magnetization in the c direction for any temperature.

    Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×