Magnetic spin order in the honeycomb structured Pb6Co9(TeO6)5 compound

I. Panneer Muthuselvam, K. Saranya, Deepa Kasinathan, R. N. Bhowmik, R. Sankar, Namasivayam Dhenadhayalan, G. J. Shu, Wei-tin Chen, L. Kavitha, and King-Chuen Lin
Phys. Rev. B 104, 174442 – Published 29 November 2021
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Abstract

We present a comprehensive experimental and theoretical study of the structural, electronic, magnetic, and thermodynamic properties of a Pb6Co9(TeO6)5 single crystal. The Pb6Co9(TeO6)5 crystal has shown a unique type of magnetic spin-lattice coupling, in which the lattice structure consists of four different Co ions sites with distorted octahedral coordinations. The x-ray photoelectron spectroscopy (XPS) results confirmed the oxidation states of Pb, Co, Te, and O elements in the sample. Moreover, XPS spectra revealed the adsorbed oxygen in the defect/vacancy sites of the lattice structure. The dc magnetization measurements exhibited a complex magnetic behavior with ferrimagnetic (FIM) transition with Curie temperature TC at 21 K. At lower magnetic fields H, the zero-field-cooled and field-cooled curves showed a broad hump at 10.8 K and a shoulder peak at 6.2 K, which are suppressed at higher magnetic fields. The ac susceptibility data indicated spin-glass-like features. The heat capacity CP measurements confirmed the FIM transition at TC at 21 K, but without any trace of additional peaks at lower temperatures. The estimated Curie-Weiss constant θCW showed a peculiar field-dependent behavior along the Hc direction of the single crystal, where θCW is less field dependent for the Hc direction. A large coercivity (13 kOe) is observed at 2 K for Hc, whereas the magnetization curve of the single crystal is dominated by an antiferromagnetic feature for Hc. The behaviors indicate the anisotropy nature of the exchange interactions in the compound. The local spin density approximation + U total energy calculations were performed for various collinear spin configurations of a classical Heisenberg model in order to obtain the magnetic exchange interactions Ji at different distances for different neighbors.

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  • Received 28 January 2021
  • Revised 2 September 2021
  • Accepted 15 November 2021

DOI:https://doi.org/10.1103/PhysRevB.104.174442

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

I. Panneer Muthuselvam1,*, K. Saranya2, Deepa Kasinathan3, R. N. Bhowmik4,†, R. Sankar5,6, Namasivayam Dhenadhayalan7, G. J. Shu6,8, Wei-tin Chen6, L. Kavitha2, and King-Chuen Lin7

  • 1Department of Physics (MMV), Banaras Hindu University, Varanasi 221005, Uttar Pradesh, India
  • 2Department of Physics, School of Basic and Applied Sciences, Central University of Tamil Nadu, Neelakudi, Thiruvarur 610005, Tamil Nadu, India
  • 3Max-Planck Institute for Chemical Physics of Solids, Nöthnitzer Strasse 4001187 Dresden, Germany
  • 4Department of Physics, Pondicherry University, R. Venkataraman Nagar, Kalapet, Pondicherry 605014, India
  • 5Institute of Physics, Academia Sinica, Taipei 10617, Taiwan
  • 6Center for Condensed Matter Sciences, National Taiwan University, Taipei 10617, Taiwan
  • 7Department of Chemistry, National Taiwan University, and Institute of Atomic and Molecular Sciences, Academia Sinica, Taipei 10617, Taiwan
  • 8Department of Materials and Mineral Resources Engineering, Institute of Mineral Resources Engineering, National Taipei University of Technology, Taipei 10608, Taiwan

  • *ipmphysics@gmail.com
  • rnbhowmik.phy@pondiuni.edu.in

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Issue

Vol. 104, Iss. 17 — 1 November 2021

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