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

ORAL

Abstract

HgCr2Se4 is a well-known ferromagnetic(FM) semiconductor with TC = 106 ~ 120 K1 and it has received renewed interest recently. Here, we performed the first comprehensive high-pressure study on n-type HgCr2Se4 single crystals and surprisingly found that the FM metallic ground state is destabilized and gradually replaced by an antiferromagnetic (AF) insulating ground state under high pressure. Our combined magnetic susceptibility and neutron measurements under high pressure indicated that the AF order is most likely a spiral-type. On the other hand, the application of external magnetic fields can restore the FM metallic state again at high pressures, resulting in a colossal magnetoresistance as high as ~ 3 ^ 1011 % under 5 T and 2 K at 4 GPa. Our results demonstrate that HgCr2Se4 situates at a critical point where the competition between FM and AF exchange interactions can be easily tuned by pressure and magnetic field. Thus, our work provides a means for realizing novel state where the extremely large magnetoresistance can be obtained via switching between two distinct electronic ground states in a single-valent system2.
1. P. K. Baltzer et al., Phys. Rev. Lett. 1965, 15, 493
2. J. P. Sun et al., Phys. Rev. Lett. 2019, 123, 047201

Presenters

  • Jianping Sun

    Institute of Physics, Chinese Academy of Sciences

Authors

  • Jianping Sun

    Institute of Physics, Chinese Academy of Sciences

  • Yuanyuan Jiao

    Institute of Physics, Chinese Academy of Sciences

  • Sachith Dissanayake

    Department of Physics, Duke University, Department of Physics, Duke University, Durham, North Carolina, USA, Physics, Duke University, Oak Ridge National Lab, Duke University, Oak Ridge National Laboratory

  • Masaaki Matsuda

    Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge National Laboratory, Oak Ridge National Lab

  • Yoshiya Uwatoko

    Institute for Solid State Physics, University of Tokyo, Institute for Solid State Physics, The University of Tokyo, Institute for Solid State Physics, Univ of Tokyo

  • Youguo Shi

    Chinese Academy of Sciences, Institute of Physics, Chinese Academy of Sciences

  • Yongqing Li

    Institute of Physics, Chinese Academy of Sciences, Chinese Academy of Sciences

  • Zhong Fang

    Institute of Physics, Chinese Academy of Sciences

  • Jinguang Cheng

    Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Chinese Academy of Sciences,Institute of Physics, Institute of Physics, Chinese Academy of Sciences