We investigate the non-Fermi liquid (NFL) behaviors at the two-dimensional (2D) magnetic heterostructure interface between a normal metal and a magnetic insulator. The normal metal undergoes a Lifshitz transition with van Hove singularities (VHS) saddle points tuned onto the Fermi surface, which represents a convex-to-concave geometric transition of the 2D Fermi surface. By coupling to critical spin fluctuations via interfacial exchange interactions, we uncover a novel NFL phase at the VHS with the quasiparticle lifetime scaling as ~ ω1/2. This NFL feature dominates over the rest of the Fermi surface points in the low-energy limit. At finite energies, it crossovers to the marginal Fermi liquid. Importantly, we demonstrate the strange metal behaviors, that includes the linear-in-T resistivity and the Tln (1/T) specific heat, already present with the spatially uniform interaction, which broadens the scenario in {https://www.science.org/doi/abs/10.1126/science.abq6011}{Science { 381}, 790 (2023)}. Furthermore, we propose the non-magnetic ARPES can directly probe the NFL features at heterostructure interface. Our findings explore the interplay of VHS in lower dimension, disorder and strong interactions, which paves a novel path to study the quantum critical phenomenon, 2D magnetism and spintronics.
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Xing et al. (2024) studied this question.
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