<p>We revisit 6d (2,0) SCFTs of type <i>D</i><sub><i>N</i></sub> and their realization in M-theory, focusing on absolute variants of these theories and on their global finite 0- and 2-form symmetries. We derive the 7d SymTFT capturing these global symmetries from M-theory, both from the point of view of the low-energy supergravity action on <b>AdS</b><sub>7</sub> × <b>RP</b><sup>4</sup> and from M2- and M5-branes giving rise to its topological operators. Along the way, results by Gukov, Hsin, and Pei are extended by keeping track of an additional 7d <i>ℤ</i><sub>2</sub> gauge field, associated to the outer automorphism of the <i>D</i><sub><i>N</i></sub> algebra. In particular, we find an interplay of non-invertible symmetries and mixed anomalies for absolute 6d (2,0) <i>D</i><sub>4<i>k</i></sub> SCFTs with <i>k</i> ≥ 1. We highlight several subtle points related to the non-orientability of <b>RP</b><sup>4</sup>, the half-integral <i>G</i><sub>4</sub>-flux that threads it, and the non-commutativity of fluxes. All these also play an essential role in a holographic derivation of the anomaly polynomial of 6d (2,0) <i>D</i><sub><i>N</i></sub> SCFTs.</p>

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SymTFTs and non-invertible symmetries of 6d (2,0) SCFTs of type D from M-theory

  • Federico Bonetti,
  • Michele Del Zotto,
  • Ruben Minasian

摘要

We revisit 6d (2,0) SCFTs of type DN and their realization in M-theory, focusing on absolute variants of these theories and on their global finite 0- and 2-form symmetries. We derive the 7d SymTFT capturing these global symmetries from M-theory, both from the point of view of the low-energy supergravity action on AdS7 × RP4 and from M2- and M5-branes giving rise to its topological operators. Along the way, results by Gukov, Hsin, and Pei are extended by keeping track of an additional 7d 2 gauge field, associated to the outer automorphism of the DN algebra. In particular, we find an interplay of non-invertible symmetries and mixed anomalies for absolute 6d (2,0) D4k SCFTs with k ≥ 1. We highlight several subtle points related to the non-orientability of RP4, the half-integral G4-flux that threads it, and the non-commutativity of fluxes. All these also play an essential role in a holographic derivation of the anomaly polynomial of 6d (2,0) DN SCFTs.