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Antiferromagnetic order in single crystals of the S=2 quasi-one-dimensional chain MnCl3(bpy)

Shin-ichi Shinozaki, Akira Okutani, Daichi Yoshizawa, Takanori Kida, Tetsuya Takeuchi, Shoji Yamamoto, Olivia N. Risset, Daniel R. Talham, Mark W. Meisel, and Masayuki Hagiwara
Phys. Rev. B 93, 014407 – Published 8 January 2016

Abstract

A suite of experimental tools, including high-field magnetization and electron spin resonance (ESR) studies in magnetic fields of up to 50 T and heat capacity studies up to 9 T, have revealed antiferromagnetic order in single crystals of the Heisenberg S=2 chain compound MnCl3(bpy), where bpy is 2,2-bipyridine. The Néel temperature, which depends on the strength of the applied magnetic field and its orientation with respect to the crystalline axes that was revealed by heat capacity measurements, is near 11.5 K in zero field. The spin-flop transition is identified in the magnetization curve acquired at 1.7 K and at μoHSFc=24 T along the c axis. The transition field HSF is lower than that expected from the previous antiferromagnetic resonance (AFMR) studies on a powder sample. The identification of the long-range antiferromagnetic order resolves an earlier report by Granroth et al. [Phys. Rev. Lett. 77, 1616 (1996)] that identified MnCl3(bpy) as an S=2 Haldane system down to 40 mK. The ESR studies identify a wide range of antiferromagnetic resonance modes that provide additional microscopic information about the g values (ga*=2.09, gb=1.92, and gc=2.07), the zero-field splitting constants, D/kB=1.5 K and E/kB=0.17 K when the nearest-neighbor spin interaction J/kB=31.2 K, which is evaluated from fitting the susceptibility, and the anisotropy of this compound (easy axis is the c axis, the second easy-axis is the b axis, and the hard axis is the a* axis), when using a standard (two-sublattice) AFMR analysis that does not quantitatively reproduce the observed HSFc value. The observed resonance mode indicates the frequency minimum at HSFc.

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  • Received 2 November 2015

DOI:https://doi.org/10.1103/PhysRevB.93.014407

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Shin-ichi Shinozaki1, Akira Okutani1, Daichi Yoshizawa1, Takanori Kida1, Tetsuya Takeuchi2, Shoji Yamamoto3, Olivia N. Risset4, Daniel R. Talham4, Mark W. Meisel5, and Masayuki Hagiwara1,*

  • 1Center for Advanced High Magnetic Field Science, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan
  • 2Low Temperature Center, Osaka University, Toyonaka, Osaka 560-0043, Japan
  • 3Department of Physics, Hokkaido University, Sapporo, Hokkaido 060-0810, Japan
  • 4Department of Chemistry, University of Florida, Gainesville, Florida 32611-7200, USA
  • 5Department of Physics and the National High Magnetic Field Laboratory, University of Florida, Gainesville, Florida 32611-8440, USA

  • *Corresponding author: hagiwara@ahmf.sci.osaka-u.ac.jp

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Issue

Vol. 93, Iss. 1 — 1 January 2016

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