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Paradigm cases with exact higher-form symmetries

The argument

Where a generalized symmetry is exact, its realization is a sharp, discrete label that cannot change without nonanalytic behavior, just as for ordinary symmetries. Because confinement and deconfinement in pure Yang-Mills correspond to distinct realizations of the center one-form symmetry, and because topological order corresponds to spontaneous breaking of higher-form symmetries, distinct realizations of generalized symmetries demonstrably label distinct phases in the two paradigm settings, gauge theory and gapped condensed matter.

Does it work?

Not yet evaluated.

Premises

Where it is made

Passages where sources make, criticize or mention this argument. They record where it appears, not how strong it is, and none has precedence over another.

No source is recorded as making it.

Earlier ratings

  • Aug 4, 2026

    The inference goes through: if the paradigm identifications are correct, distinct realizations of exact generalized symmetries demonstrably label distinct phases in both gauge theory and gapped condensed matter, which is what the argument needs. Its weight rests on the Yang-Mills deconfinement case and the identification of topological order as higher-form symmetry breaking; neither has yet received its own assessment, but both rest on well-established physics, the former backed by lattice results and the latter explicit in abelian models such as the toric code. The connecting premise, that the realization of an exact symmetry is a discrete label that cannot change without nonanalyticity, is the standard Landau-type reasoning and is not disputed for exact symmetries.

Paradigm cases with exact higher-form symmetries · Minerval