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Magnetic-Competition-Induced Colossal Magnetoresistance in n-Type HgCr2Se4 under High Pressure

J. P. Sun, Y. Y. Jiao, C. J. Yi, S. E. Dissanayake, M. Matsuda, Y. Uwatoko, Y. G. Shi, Y. Q. Li, Z. Fang, and J.-G. Cheng
Phys. Rev. Lett. 123, 047201 – Published 22 July 2019
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Abstract

The n-type HgCr2Se4 exhibits a sharp semiconductor-to-metal transition (SMT) in resistivity accompanying the ferromagnetic order at TC=106K. Here, we investigate the effects of pressure and magnetic field on the concomitant SMT and ferromagnetic order by measuring resistivity, dc and ac magnetic susceptibility, as well as single-crystal neutron diffraction under various pressures up to 8 GPa and magnetic fields up to 8 T. Our results demonstrate that the ferromagnetic metallic ground state of n-type HgCr2Se4 is destabilized and gradually replaced by an antiferromagnetic, most likely a spiral magnetic, and insulating ground state upon the application of high pressure. On the other hand, the application of external magnetic fields can restore the ferromagnetic metallic state again at high pressures, resulting in a colossal magnetoresistance (CMR) as high as 3×1011% under 5 T and 2 K at 4 GPa. The present study demonstrates that n-type HgCr2Se4 is located at a peculiar critical point where the balance of competition between ferromagnetic and antiferromagnetic interactions can be easily tipped by external stimuli, providing a new platform for achieving CMR in a single-valent system.

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  • Received 25 March 2019

DOI:https://doi.org/10.1103/PhysRevLett.123.047201

© 2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

J. P. Sun1,2, Y. Y. Jiao1,3, C. J. Yi1,2, S. E. Dissanayake4,5, M. Matsuda4, Y. Uwatoko6, Y. G. Shi1,2,7, Y. Q. Li1,2,7, Z. Fang1,2,7, and J.-G. Cheng1,2,7,*

  • 1Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100190, China
  • 3Faculty of Science, Wuhan University of Science and Technology, Wuhan, Hubei 430065, China
  • 4Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 5Department of Physics, Duke University, Durham, North Carolina 27708, USA
  • 6Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581, Japan
  • 7Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China

  • *jgcheng@iphy.ac.cn

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Vol. 123, Iss. 4 — 26 July 2019

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Images

  • Figure 1
    Figure 1

    (a)–(i) Temperature dependence of resistivity ρ(T) of HgCr2Se4 at 0 and 8 T under various pressures up to 7 GPa.

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  • Figure 2
    Figure 2

    Temperature dependence of resistivity ρ(T) and MR ratio at different magnetic fields (ZFC) under various represented pressures: (a) 2, (b) 3, (c) 4, and (d) 7 GPa. In (a)–(d) and (e)–(h), the resistivity ρ(T) and MR have the same coordinate range as in (a) and (e).

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  • Figure 3
    Figure 3

    (a),(b) Temperature dependence of dc and ac susceptibility of HgCr2Se4 under high pressures. The ferromagnetic transition temperatures TC and the antiferromagnetic transition temperatures TN are marked by arrows. (c) Temperature dependence of the integrated intensities of the (111) Bragg peak observed by neutron diffraction at 0, 1.5, and 3.0 GPa. The intensities between different pressures are normalized using the (111) nuclear Bragg peak intensities above TC.

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  • Figure 4
    Figure 4

    Temperature-pressure phase diagram of n-type HgCr2Se4. The ferromagnetic ordering temperatures (TC, black filled circle, green triangle, and brown pentagon), the upturn in resistivity (Tmin, blue square), and the spiral magnetic ordering temperatures (TN, red rhombus) as a function of hydrostatic pressure.

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