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High-temperature magnetostructural transition in van der Waals-layered αMoCl3

Michael A. McGuire, Jiaqiang Yan, Paula Lampen-Kelley, Andrew F. May, Valentino R. Cooper, Lucas Lindsay, Alexander Puretzky, Liangbo Liang, Santosh KC, Ercan Cakmak, Stuart Calder, and Brian C. Sales
Phys. Rev. Materials 1, 064001 – Published 7 November 2017

Abstract

The crystallographic and magnetic properties of the cleavable 4d3 transition metal compound αMoCl3 are reported, with a focus on the behavior above room temperature. Crystals were grown by chemical vapor transport and characterized using temperature dependent x-ray diffraction, Raman spectroscopy, and magnetization measurements. A structural phase transition occurs near 585 K, at which the Mo-Mo dimers present at room temperature are broken. A nearly regular honeycomb net of Mo is observed above the transition, and an optical phonon associated with the dimerization instability is identified in the Raman data and in first-principles calculations. The crystals are diamagnetic at room temperature in the dimerized state, and the magnetic susceptibility increases sharply at the structural transition. Moderately strong paramagnetism in the high-temperature structure indicates the presence of local moments on Mo. This is consistent with results of spin-polarized density functional theory calculations using the low- and high-temperature structures. Above the magnetostructural phase transition the magnetic susceptibility continues to increase gradually up to the maximum measurement temperature of 780 K, with a temperature dependence that suggests two-dimensional antiferromagnetic correlations.

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  • Received 10 August 2017

DOI:https://doi.org/10.1103/PhysRevMaterials.1.064001

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Michael A. McGuire1,*, Jiaqiang Yan1, Paula Lampen-Kelley1, Andrew F. May1, Valentino R. Cooper1, Lucas Lindsay1, Alexander Puretzky2, Liangbo Liang2, Santosh KC1, Ercan Cakmak1, Stuart Calder3, and Brian C. Sales1

  • 1Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 2Center for Nanophase Materials Science, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3Quantum Condensed Matter Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

  • *McGuireMA@ornl.gov

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Issue

Vol. 1, Iss. 6 — November 2017

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Images

  • Figure 1
    Figure 1

    (a) Crystals of αMoCl3 grown by vapor transport. (b) DSC thermal signatures of the reversible phase transition near 585 K. (c) Rietveld fits to x-ray diffraction data collected at 300 and 623 K with honeycomb Mo nets shown in the insets. The upper set of ticks denote reflections from AlCl3-type MoCl3 and the lower set correspond to the silicon powder that was mixed with the sample.

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  • Figure 2
    Figure 2

    The crystal structures of αMoCl3 determined at 300 and 623 K. (a) A single layer viewed along the stacking direction. The dimers present in the distorted honeycomb net of Mo at 300 K are indicated by the thick black lines. (b) A single layer viewed normal to the stacking direction. Dimers are indicated by thick black lines, and dashed lines are drawn through the Cl layers to highlight the buckling out of Cl atoms between the dimerized Mo atoms as indicated by the arrows. (c) Coordination polyhedra around a single Mo-Mo pair, showing the off-centering of the Mo atoms at 300 K and the associated bending of the apical Cl-Mo-Cl chain and slight twisting distortion of the octahedra.

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  • Figure 3
    Figure 3

    Temperature dependence of the structural parameters determined from diffraction measurements on αMoCl3. (a) The a and b lattice parameters. (b) The c lattice parameter and monoclinic angle β. (c) The layer spacing corresponding to the perpendicular distance between midpoints of neighboring layers and the unit cell volume. (d) The nearest-neighbor MoMo distances d1 and d2 as defined in Fig. 1, and the y coordinate of Mo. Results from a second sample at 300, 600, and 623 K are also shown.

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  • Figure 4
    Figure 4

    Results of Raman spectroscopy measurements on αMoCl3. (a) Spectra collected at the temperatures indicated on the plot, offset vertically. (b) Temperature dependence of the Raman shifts and intensities relative to 297 K values for modes 1, 2, and 3 labeled in (a). (c) Atomic displacements corresponding to modes 1, 2, and 3.

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  • Figure 5
    Figure 5

    The crystallographic phase transition in αMoCl3 probed by magnetization measurements. (a) Magnetic susceptibility χ=M/H of MoCl3 crystals measured in an applied field of 50 kOe. (b) Isothermal magnetization curves at selected temperatures. (c) Susceptibility determined upon heating and cooling through the phase transition region.

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