We investigate the interplay between (-1)-form symmetries and their quantum-dual (d - 1)-form counterparts within the framework of Symmetry Topological Field Theories (SymTFTs). In this framework the phenomenon of decomposition - a d-dimensional quantum field theory with (d - 1)-form symmetry being the disjoint union of other theories (or "universes") - arises naturally from manipulations of topological boundary conditions of the SymTFT. We corroborate our findings with various examples, including a generalization of "instanton-restricted" 4d Yang-Mills theories with no sum over instanton sectors. Furthermore, we construct a 3d SymTFT with a non-invertible (-1)-form symmetry. The absolute 2d quantum field theory includes a 0-form global symmetry that depends on a parameter whose value gets shifted by the action of the (-1)-form symmetry, and we show that the non-invertibility of the latter is needed to encode this modification of the 0-form symmetry.
Lin, L., Robbins, D., Roy, S. (2025). Decomposition and (non-invertible) (−1)-form symmetries from the symmetry topological field theory. JOURNAL OF HIGH ENERGY PHYSICS, 2025(9), 1-43 [10.1007/JHEP09(2025)131].
Decomposition and (non-invertible) (−1)-form symmetries from the symmetry topological field theory
Lin L.;
2025
Abstract
We investigate the interplay between (-1)-form symmetries and their quantum-dual (d - 1)-form counterparts within the framework of Symmetry Topological Field Theories (SymTFTs). In this framework the phenomenon of decomposition - a d-dimensional quantum field theory with (d - 1)-form symmetry being the disjoint union of other theories (or "universes") - arises naturally from manipulations of topological boundary conditions of the SymTFT. We corroborate our findings with various examples, including a generalization of "instanton-restricted" 4d Yang-Mills theories with no sum over instanton sectors. Furthermore, we construct a 3d SymTFT with a non-invertible (-1)-form symmetry. The absolute 2d quantum field theory includes a 0-form global symmetry that depends on a parameter whose value gets shifted by the action of the (-1)-form symmetry, and we show that the non-invertibility of the latter is needed to encode this modification of the 0-form symmetry.| File | Dimensione | Formato | |
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