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    Single-crystalline orthorhombic GdAlGe as a rare-earth magnetic Dirac nodal-line metal

    Antu Laha1,2,*,†, Juntao Yao2,3,*, Asish K. Kundu4,*,‡, Niraj Aryal2,*,§, Anil Rajapitamahuni4, Elio Vescovo4, Fernando Camino5, Kim Kisslinger5, Lihua Zhang5 et al.

    Dmytro Nykypanchuk5, J. Sears2, J. M. Tranquada2, Weiguo Yin2, and Qiang Li1,2,∥

    • *These authors contributed equally to this work.
    • †Contact author: antulaha.physics@gmail.com
    • ‡Contact author: akundu@bnl.gov
    • §Contact author: naryal@bnl.gov
    • ∥Contact author: liqiang@bnl.gov

    Phys. Rev. B 112, 125155 – Published 24 September, 2025

    DOI: https://doi.org/10.1103/r7gz-kwqw

    Abstract

    Crystal engineering is a method for discovering new quantum materials and phases, which may be achieved using external pressure or strain. Chemical pressure is unique in that it generates internal pressure perpetually to the lattice. As an example, GdAlSi from the rare-earth (R) RAlX (X=Si or Ge) family of Weyl semimetals is considered. Replacing Si with the larger isovalent element Ge creates sufficiently large chemical pressure to induce a structural transition from the tetragonal structure of GdAlSi, compatible with a Weyl semimetallic state, to an orthorhombic phase in GdAlGe, resulting in an inversion-symmetry-protected nodal-line metal. We find that GdAlGe hosts an antiferromagnetic ground state with two successive orderings, at TN1=35K and TN2=30K. In-plane isothermal magnetization shows a magnetic field induced metamagnetic transition at 6.2 T for 2 K. Furthermore, electron-hole compensation gives rise to a large magnetoresistance of ∼100% at 2 K and 14 T. Angle-resolved photoemission spectroscopy measurements and density functional theory calculations reveal a Dirac-like linear band dispersion over an exceptionally large energy range of ∼1.5eV with a high Fermi velocity of ∼106 m/s, a rare feature not observed in any magnetic topological materials.

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