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Staggered Fermions with Chiral Anomaly Cancellation

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arxiv 2501.10837 v2 pith:Q3SRAZCE submitted 2025-01-18 hep-lat cond-mat.str-elhep-phhep-th

classification hep-latcond-mat.str-elhep-phhep-th
keywords latticefermionschargeschiralcontinuumdiracanomalymass
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abstract

We investigate the implications of the quantized vectorial and axial charges in the lattice Hamiltonian of multi-flavor staggered fermions in $(1+1)$ dimensions. These lattice charges coincide with those of the $U(1)_V$ and $U(1)_A$ global symmetries of Dirac fermions in the continuum limit, whose perturbative chiral anomaly matches the non-Abelian Onsager algebra on the lattice. In this note, we focus on the lattice models that flow to continuum quantum field theories of Dirac fermions that are free from the perturbative chiral anomaly between $U(1)_V$ and $U(1)_A$. In a lattice model that flows to two Dirac fermions, we identify quadratic Hamiltonian deformations that can gap the system while fully preserving both the vectorial and axial charges on the lattice. These deformations flow to the usual symmetry-preserving Dirac mass terms in the continuum. Additionally, we propose a lattice model that flows to the chiral fermion $3-4-5-0$ model in the continuum by using these lattice charges, and we discuss the multi-fermion interactions that can generate a mass gap in the paradigm of symmetric mass generation.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Fermionic Villain model with exact lattice chiral symmetries

    hep-th 2026-08 conditional novelty 7.0 of 10

    A fermionic Villain lattice Hamiltonian exactly realizes the chiral U(1) L x U(1) R symmetry and anomalies of a massless Dirac fermion, enabling exact studies of symmetric mass generation and chiral lattice gauge theories.

  2. Non-singlet conserved charges and anomalies in 3+1 D staggered fermions

    hep-lat 2025-09 conditional novelty 7.0 of 10

    The 3+1D staggered fermion Hamiltonian has conserved charges generating SU(2)_A in the continuum, and their mixed lattice anomaly with the vector charge becomes trivial once the continuum QFT is reached.

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