Mn(Pt1xPdx)5P: Isovalent tuning of Mn-sublattice magnetic order

Tyler J. Slade, Ranuri S. Dissanayaka Mudiyanselage, Nao Furukawa, Tanner R. Smith, Juan Schmidt, Lin-Lin Wang, Chang-Jong Kang, Kaya Wei, Zhixue Shu, Tai Kong, Ryan Baumbach, Gabriel Kotliar, Sergey L. Bud'ko, Weiwei Xie, and Paul C. Canfield
Phys. Rev. B 107, 134429 – Published 21 April 2023

Abstract

We report the growth and characterization of MnPd5P, a rare-earth-free ferromagnet, with TC295K and planar anisotropy, and conduct a substitutional study with its antiferromagnetic analog MnPt5P. All compounds in the family adopt the layered anti-CeCoIn5-type structure with the space group P4/mmm, and EDS and x-ray diffraction results indicate that MnPt5P and MnPd5P form a complete solid solution. Based on measurements of the temperature- and field-dependent magnetization and resistance, we construct a temperature-composition (Tx) phase diagram for Mn(Pt1xPdx)5P and demonstrate that the essentially antiferromagnetic order found in MnPt5P is extraordinarily sensitive to Pd substitution. At low Pd fractions (x<0.010), the single antiferromagnetic-like transition in pure MnPt5P splits into a higher-temperature ferromagnetic transition followed first, upon cooling, by a lower temperature ferromagnetic to antiferromagnetic transition and then by a re-entrant antiferromagnetic to ferromagnetic transition at even lower temperatures. The antiferromagnetic region makes up a bubble phase that persists up to x0.008–0.009 for T150K, with all samples 0x<0.008 recovering their initial ferromagnetic state upon further cooling to base temperature. Once x>0.010, Mn(Pt1xPdx)5P undergoes a only single transition into the ferromagnetic phase. The Curie temperature initially increases rapidly with x, rising from TC197K at x = 0.013 to a maximum of TC312K for x0.62, and then falling back to TC295K for pure MnPd5P (x=1.00). Given that Pt and Pd are isoelectronic, this work raises questions as to the origin of the extreme sensitivity of the magnetic ground state and the nature of the re-entrant ferromagnetism at dilute Pd levels.

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  • Received 28 October 2022
  • Revised 21 February 2023
  • Accepted 24 March 2023

DOI:https://doi.org/10.1103/PhysRevB.107.134429

©2023 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Tyler J. Slade1,2,*,†, Ranuri S. Dissanayaka Mudiyanselage3,*, Nao Furukawa1,2, Tanner R. Smith1,2, Juan Schmidt1,2, Lin-Lin Wang1, Chang-Jong Kang4,5, Kaya Wei6, Zhixue Shu7, Tai Kong7, Ryan Baumbach6, Gabriel Kotliar4, Sergey L. Bud'ko1,2, Weiwei Xie3,8, and Paul C. Canfield1,2,‡

  • 1Ames National Laboratory, US DOE, Iowa State University, Ames, Iowa 50011, USA
  • 2Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
  • 3Department of Chemistry and Chemical Biology, The State University of New Jersey Rutgers, Piscataway, New Jersey 08854, USA
  • 4Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey, 08854, USA
  • 5Department of Physics, Chungnam National University, Daejeon, 34134, South Korea
  • 6National High Magnetic Field Laboratory, Tallahassee, Florida, 32310, USA
  • 7Department of Physics, University of Arizona, Tucson, Arizona 85721, USA
  • 8Department of Chemistry, Michigan State University, East Lansing, Michigan, 48824, USA

  • *These authors contributed equally to this work.
  • slade@ameslab.gov
  • canfield@ameslab.gov

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Issue

Vol. 107, Iss. 13 — 1 April 2023

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