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Parity Anomaly and Duality Web

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abstract

We review the parity anomaly and a duality web in 2+1 dimensions. An odd dimensional non-interacting Dirac fermion theory is not parity invariant at quantum level. We demonstrate the parity anomaly in a three dimensional non-interacting Dirac fermion theory and a one dimensional non-interacting Dirac fermion theory. These theories can generate non-gauge invariant Abelian Chern-Simons terms at a finite temperature through an effective action. The parity anomaly also leads us to study the duality web in 2+1 dimensions, in which the 2+1 dimensional duality web begins from the conjecture of a duality between a three dimensional Dirac fermion theory and a three dimensional interacting scalar field theory at the Wilson-Fisher fixed point. We first review the duality web for the flat background, then we discuss its extension to the spin$_c$ manifold to avoid inconsistency from the spin structure. This also leads a global effect. We discuss that the composite fermions approach of the quantum Hall system also suffers from the same issue of the global description. Finally, we use perspective of the electric-magnetic duality of the Abelian gauge theory in 3+1 dimensions to study the 2+1 dimensional duality web.

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fields

hep-lat 1

years

2026 1

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CONDITIONAL 1

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background 1

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unclear 1

representative citing papers

Chemical Potential and Analytic Continuation for Non-Hermitian Lattice Fermions

hep-lat · 2026-08-09 · conditional · novelty 3.0

For a one-dimensional free non-Hermitian lattice fermion, the finite-lattice propagator is analytic in the chemical potential, the infinite-volume/continuum limit can destroy that analyticity, and paired potentials (μ,-μ) or (iμ,iμ) make Hybrid Monte Carlo sign-problem-free.

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  • Chemical Potential and Analytic Continuation for Non-Hermitian Lattice Fermions hep-lat · 2026-08-09 · conditional · none · ref 29 · internal anchor

    For a one-dimensional free non-Hermitian lattice fermion, the finite-lattice propagator is analytic in the chemical potential, the infinite-volume/continuum limit can destroy that analyticity, and paired potentials (μ,-μ) or (iμ,iμ) make Hybrid Monte Carlo sign-problem-free.