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Higher symmetries, anomalies, and crossed squares in lattice gauge theory

3 Pith papers cite this work. Polarity classification is still indexing.

3 Pith papers citing it

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2026 2 2025 1

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UNVERDICTED 3

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$K$-Theoretic Obstructions to Linearizing QCA Representations

math.AT · 2026-06-17 · unverdicted · novelty 7.0

Develops K-theoretic obstruction theory for linearizing QCA representations over arbitrary fields, extracting universal classes and computing homotopy types over point/line/plane in the complex unitary case.

Infinite-Order Lattice Chiral Anomalies and CPT

hep-th · 2026-06-10 · unverdicted · novelty 7.0

Lattice CPT symmetry upgrades the Onsager chiral symmetry anomaly from order two to infinite order, better matching the continuum chiral anomaly, with discussion of associated 2+1d SPT phases.

Onsiteability of Higher-Form Symmetries

cond-mat.str-el · 2025-10-27 · unverdicted · novelty 6.0

For finite 1-form symmetries in (2+1)D, onsiteability holds exactly when the 't Hooft anomaly meets an algebraic condition allowing 1-gauging; the symmetry can then be realized as transversal Pauli operators via ancillas and circuits.

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Showing 3 of 3 citing papers after filters.

  • $K$-Theoretic Obstructions to Linearizing QCA Representations math.AT · 2026-06-17 · unverdicted · none · ref 12

    Develops K-theoretic obstruction theory for linearizing QCA representations over arbitrary fields, extracting universal classes and computing homotopy types over point/line/plane in the complex unitary case.

  • Infinite-Order Lattice Chiral Anomalies and CPT hep-th · 2026-06-10 · unverdicted · none · ref 24

    Lattice CPT symmetry upgrades the Onsager chiral symmetry anomaly from order two to infinite order, better matching the continuum chiral anomaly, with discussion of associated 2+1d SPT phases.

  • Onsiteability of Higher-Form Symmetries cond-mat.str-el · 2025-10-27 · unverdicted · none · ref 5

    For finite 1-form symmetries in (2+1)D, onsiteability holds exactly when the 't Hooft anomaly meets an algebraic condition allowing 1-gauging; the symmetry can then be realized as transversal Pauli operators via ancillas and circuits.