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Anomaly Constraints on Gapped Phases with Discrete Chiral Symmetry

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arxiv 1912.13069 v1 pith:JF3ZWZ42 submitted 2019-12-30 hep-th cond-mat.str-elmath-phmath.ATmath.MP

classification hep-thcond-mat.str-elmath-phmath.ATmath.MP
keywords symmetrytheoriescertainchiraldiscretefieldgappedphases
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abstract

We prove that in $(3+1)d$ quantum field theories with $\mathbb{Z}_N$ symmetry, certain anomalies forbid a symmetry-preserving vacuum state with a gapped spectrum. In particular, this applies to discrete chiral symmetries which are frequently present in gauge theories as we illustrate in examples. Our results also constrain the long-distance behavior of certain condensed matter systems such as Weyl-semimetals and may have applications to crystallographic phases with symmetry protected topological order. These results may be viewed as analogs of the Lieb-Schultz-Mattis theorem for continuum field theories.

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Cited by 6 Pith papers

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

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    Generalized family anomalies for broken higher-group and non-invertible symmetries constrain RG flows and IR phases of QFT families, with explicit application to deformed 4d QCD.

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    Finite-group-enriched 3+1d topological orders are classified by 2SVect-enriched G-crossed braided fusion 2-categories, with gauging obstructions living in SW^5(BG).

  3. SymTFT, Protected Gaplessness, and Spontaneous Breaking of Non-invertible Symmetries

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    From anomaly cancellation plus a stipulated minimality principle, the Standard Model is forced to N_c=N_f=3; the paper proves supporting theorems: H^d(Z_n,U(1)) cocycles split under the Z_n→Z_{n^2} extension, while A_...

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    hep-th 2025-06 conditional novelty 4.0 of 10

    Explicit integer-valued anomaly indices for 4d Weyl fermions with Spin×Z_n and Spin×_{Z_2^F} Z_{2m} symmetries are derived from restriction of continuous U(1) anomalies and η-invariant evaluations.

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