How do higher-form symmetries affect anomaly matching in gauge theories?

Higher-form global symmetries generalize ordinary symmetries by acting on extended operators such as lines or surfaces rather than local fields. Davide Gaiotto at Perimeter Institute and Nathan Seiberg at Institute for Advanced Study framed this concept within quantum field theory, showing that these symmetries carry conserved charges supported on codimension-k manifolds and can possess their own anomalies. Understanding how these anomalies constrain low-energy physics extends the classic idea of anomaly matching pioneered for ordinary global symmetries to a wider class of constraints.

What higher-form symmetries are

A higher-form symmetry of degree p acts on p-dimensional operators. The canonical example in gauge theory is the one-form center symmetry of an SU(N) Yang-Mills theory which acts on Wilson line operators. Such symmetries can be exact, spontaneously broken, or explicitly broken by matter. They are characterized by background gauge fields that are differential forms of higher degree and by obstruction classes that record possible anomalies.

Anomalies and matching

Anomalies involving higher-form symmetries appear as mixed obstruction classes between different symmetry backgrounds or as failure of gauge invariance under large background transformations. The principle of anomaly matching remains: anomalies computed in the ultraviolet must be realized in the infrared either through massless excitations, topological quantum field theory sectors, or symmetry-breaking patterns. Practically, a mixed anomaly between a 0-form flavor symmetry and a 1-form center symmetry forbids a trivially gapped, symmetric vacuum. The modern language treats these anomalies via anomaly inflow from one higher dimension or via cohomological invariants, linking UV anomalies to robust IR phenomena.

Physical consequences and examples

In confining gauge theories a preserved one-form center symmetry implies area-law behavior for Wilson loops and constrains the spectrum to lack color-charged asymptotic states. If an anomaly ties that one-form symmetry to discrete chiral symmetry, the infrared must either break one of the symmetries or host topological order that reproduces the anomaly. These constraints have practical relevance beyond particle theory: condensed matter systems with emergent higher-form symmetries classify phases with loop or membrane excitations and guide the search for fault-tolerant qubits. Depending on topology and boundary conditions, anomalies can also force domain walls carrying lower-dimensional degrees of freedom, a feature exploited in engineered materials and quantum devices.