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    High-field-induced multiferroic phases and polarization reversal in Co3TeO6 single crystals

    Chao Dong1,*, Yuting Chang1,*,†, Lingfan Yang1, Jiangtao Shi1, Congbin Liu1,2, Haowen Wang1, Ming Yang1, Chengliang Lu1, Yisheng Chai3 et al.

    Junfeng Wang1

    • *These authors contributed equally to this work.
    • †Contact author: ytchang@hust.edu.cn

    Phys. Rev. B 113, 134441 – Published 27 April, 2026

    DOI: https://doi.org/10.1103/kr9h-qcfr

    Abstract

    We report a systematic study of the magnetic and ferroelectric properties of Co3TeO6 single crystals under pulsed magnetic fields up to 60 T, revealing pronounced anisotropic magnetoelectric coupling and novel ferroelectric phenomena. For H//a, in addition to a low-field spin-flop transition at Ha1 ∼16.7 T, two additional metamagnetic transitions occur at Ha2 ∼18.3 T and Ha3 ∼57.6 T, which correlate with a distinct new ferroelectric phase exhibiting anomalous polarization reversal. An intriguing characteristic of this reversal is the formation of a large “∞”-shaped hysteresis loop, arising from polarization sign reversal during the H-falling sweep relative to the H-rising sweep. This ferroelectric response is highly dependent on the field-sweep history, indicating complex magnetoelectric behaviors in the system. In the case of H//b, successive metamagnetic transitions are observed at Hb1 ∼6.9 T, Hb2 ∼11.5 T, Hb3 ∼21.2 T, and Hb4 ∼35.8 T, with an additional transition at higher critical magnetic fields (Hb5) above 10 K. Each transition corresponds to distinct ferroelectric phases, which exhibit varying responses to the applied bias electric field (E). In particular, the high-field ferroelectric phase above Hb4 demonstrates a robust memory effect, where both the direction and magnitude of electric polarization are retained across successive pulses of −E and +E. This suggests that the pinning of ferroelectric domain walls may prevent polarization reversal under opposing bias fields. Complementary magnetostriction measurements support the magnetization results and reveal spin-lattice coupling. Based on these comprehensive experimental findings, we construct the magnetic-field-temperature phase diagrams and investigate the underlying origin of magnetoelectric coupling in Co3TeO6. Our results offer valuable insights into high-field-induced ferroelectric phases and unusual magnetoelectric effects in noncollinear multiferroic systems.

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