Absence of structural transition in M0.5IrTe2 (M = Mn, Fe, Co, Ni)

J.-Q. Yan, B. Saparov, A. S. Sefat, H. Yang, H. B. Cao, H. D. Zhou, B. C. Sales, and D. G. Mandrus
Phys. Rev. B 88, 134502 – Published 7 October 2013

Abstract

M-doped IrTe2 (M = Mn, Fe, Co, Ni) compounds were synthesized by solid-state reaction. Single crystal x-ray diffraction experiments indicate that part of the doped M ions (M = Fe, Co, and Ni) substitute for Ir, and the rest intercalate into the octahedral interstitial sites located in between IrTe2 layers. Due to the lattice mismatch between MnTe2 and IrTe2, Mn has limited solubility in IrTe2 lattice. The trigonal structure is stable in the whole temperature range 1.80 K T  300 K for all doped compositions. No long-range magnetic order or superconductivity was observed in any doped compositions above 1.80 K. A spin glass behavior below 10 K was observed in Fe-doped IrTe2 from the temperature dependence of magnetization, electrical resistivity, and specific heat. The low temperature specific heat data suggest the electron density of states is enhanced in Fe- and Co-doped compositions but reduced in Ni-doped IrTe2. With the 3d transition metal doping the trigonal a-lattice parameter increases but the c-lattice parameter decreases. Detailed analysis of the single crystal x-ray diffraction data shows that interlayer Te-Te distance increases despite a reduced c lattice. The importance of the Te-Te, Te-Ir, and Ir-Ir bonding is discussed.

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  • Received 4 August 2013

DOI:https://doi.org/10.1103/PhysRevB.88.134502

©2013 American Physical Society

Authors & Affiliations

J.-Q. Yan1,2, B. Saparov1, A. S. Sefat1, H. Yang2,3, H. B. Cao4, H. D. Zhou5, B. C. Sales1, and D. G. Mandrus1,2

  • 1Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 2Department of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA
  • 3Institute of Materials and Metallurgy, Northeastern University, Shenyang 110004, People's Republic of China
  • 4Quantum Condensed Matter Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 5Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA

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Issue

Vol. 88, Iss. 13 — 1 October 2013

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