Generalized symmetries and 2-groups via electromagnetic duality in AdS/CFT
Oliver DeWolfe, Kenneth Higginbotham
TL;DR
The paper shows that electromagnetic duality in AdS/CFT braids together gauging of generalized global symmetries and the emergence of higher-group structures in the dual field theory. By analyzing the 1-form $A_ u$ and its magnetic dual 2-form $B_{ mu u}$ in AdS$_5$, it demonstrates how regular versus alternate boundary conditions encode global versus dynamical (gauged) $U(1)$ symmetries and identify the dualized 2-form current with the field strength of the gauged $U(1)$. In a concrete example with a mixed 't Hooft anomaly, the gravity dual of a 2-group symmetry is realized via a Chern–Simons theory, and after dualizing a gauge field to a 2-form one obtains a modified field strength that matches the 2-group structure; holographic renormalization confirms the results. The framework extends naturally to general dimensions and to $n$-group symmetries, highlighting how bulk dualities provide a unifying picture for generalized symmetries in holography.
Abstract
We discuss how electromagnetically dualizing a 1-form to a 2-form in AdS$_5$ exchanges regular and alternate boundary conditions, and thus gauges the originally global $U(1)$ symmetry in the dual field theory. The generalized symmetry current dual to the 2-form in the bulk is identified as the dual field strength of the gauged $U(1)$, and the associated double-trace operator with a logarithmically running coupling is just the gauged $U(1)$ Maxwell action. Applying this dualization to an AdS Maxwell-Chern-Simons theory dual to a global $U(1) \times U(1)$ model with an 't Hooft anomaly results in a theory with a modified field strength that holographically realizes a 2-group symmetry. We explicitly carry out the holographic renormalization to verify this, and discuss the generalization to other rank fields in other dimensions.
