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    Pressure-tuned successive structural distortions and magnetic phase transitions in EuAg4As2

    Jin Jiang1,2, Xuliang Chen1,2,*, Shuyang Wang1, Chao An3, Yongji Shi1,2, Yong Nie1, Xiangde Zhu1, Wei Ning1,†, Lili Zhang4 et al.

    Yonghui Zhou1 and Zhaorong Yang1,2,3,‡

    • 1Anhui Province Key Laboratory of Low-Energy Quantum Materials and Devices, High Magnetic Field Laboratory, HFIPS, Chinese Academy of Sciences, Hefei, Anhui 230031, China
    • 2Science Island Branch, Graduate School of USTC, Hefei, Anhui 230026, China
    • 3Institutes of Physical Science and Information Technology, Anhui University, Hefei, Anhui 230601, China
    • 4Shanghai Synchrotron Radiation Facility, Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai 201204, China

    • *Contact author: xlchen@hmfl.ac.cn
    • †Contact author: ningwei@hmfl.ac.cn
    • ‡Contact author: zryang@issp.ac.cn

    Phys. Rev. B 114, 154108 – Published 18 September, 2026

    DOI: https://doi.org/10.1103/b61c-rd2y

    Abstract

    We examine the structural, vibrational, and transport properties of EuAg4As2 single crystals under pressures up to 28.8–41.8 GPa, aiming to trace the evolution of the structural distortion near TS∼130K and the two magnetic transitions at TN1∼15K and TN2∼9K. Under ambient conditions, a Raman-active phonon mode centered at ∼157cm−1 is observed and identified as having A1g symmetry, and its temperature evolution shows no discernible anomaly across these three transitions. Under pressure, combined synchrotron x-ray diffraction and Raman measurements reveal two structural distortions at PC1∼7 GPa and PC2∼17 GPa. Structural refinements and bond-valence-sum analysis suggest that these transitions mainly involve successive discontinuous modifications of the Ag-As tetrahedra, without changing the average crystal symmetry. Distinct transport and magnetic responses accompany these structural distortions: For P<PC1, TS increases while its resistivity anomaly is suppressed and TN1 and TN2 gradually increases; for PC1<P<PC1, high-temperature ferromagneticlike and low-temperature antiferromagneticlike states emerge; and for P>PC2, the resistivity becomes metalliclike, with only a faint broad kink and very weak magnetoresistance comparable to that of traditional metals.

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