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    Non-Hermitian Strongly Interacting Dirac Fermions

    Xue-Jia Yu1,2, Zhiming Pan3,4, Limei Xu1,5,6, and Zi-Xiang Li7,8,*

    • 1International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
    • 2Fujian Key Laboratory of Quantum Information and Quantum Optics, College of Physics and Information Engineering, Fuzhou University, Fuzhou, Fujian 350108, China
    • 3Department of Physics, School of Science, Westlake University, Hangzhou 310030, China
    • 4Institute for Theoretical Sciences, Westlake University, Hangzhou 310024, China
    • 5Collaborative Innovation Center of Quantum Matter, Beijing 100871, China
    • 6Interdisciplinary Institute of Light-Element Quantum Materials and Research Center for Light-Element Advanced Materials, Peking University, Beijing 100871, China
    • 7Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
    • 8School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China

    • *zixiangli@iphy.ac.cn

    Phys. Rev. Lett. 132, 116503 – Published 14 March, 2024

    DOI: https://doi.org/10.1103/PhysRevLett.132.116503

    Abstract

    Exotic quantum phases and phase transition in the strongly interacting Dirac systems have attracted tremendous interests. On the other hand, non-Hermitian physics, usually associated with dissipation arising from the coupling to environment, emerges as a frontier of modern physics in recent years. In this Letter, we investigate the interplay between non-Hermitian physics and strong correlation in Dirac-fermion systems. We generalize the projector quantum Monte-Carlo (PQMC) algorithm to the non-Hermitian interacting fermionic systems. Employing PQMC simulation, we decipher the ground-state phase diagram of the honeycomb Hubbard model with spin resolved non-Hermitian asymmetric hopping processes. The antiferromagnetic (AFM) ordering induced by Hubbard interaction is enhanced by the non-Hermitian asymmetric hopping. Combining PQMC simulation and renormalization group analysis, we reveal that the quantum phase transition between Dirac semi-metal and AFM phases belongs to Hermitian chiral XY universality class, implying that a Hermitian Gross-Neveu transition is emergent at the quantum critical point although the model is non-Hermitian.

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