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ICTP Lectures on (Non-)Invertible Generalized Symmetries

Sakura Schafer-Nameki

Non-invertible symmetries arise when a quantum field theory is stacked with topological QFTs and a diagonal symmetry is gauged, producing topological defects without inverses.

arxiv:2305.18296 v2 · 2023-05-29 · hep-th · cond-mat.str-el · hep-ph · math.CT

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Claims

C1strongest claim

The main idea that underlies many constructions of non-invertible symmetries is that of stacking a QFT with topological QFTs (TQFTs) and then gauging a diagonal non-anomalous global symmetry. The TQFTs become topological defects in the gauged theory called (twisted) theta defects.

C2weakest assumption

The foundational identification of symmetries with topological defects in a general QFT holds and extends consistently to the non-invertible case via the stacking-and-gauging construction.

C3one line summary

Lecture notes explain non-invertible generalized symmetries in QFTs as topological defects arising from stacking with TQFTs and gauging diagonal symmetries, plus their action on charges and the SymTFT framework.

References

161 extracted · 161 resolved · 23 Pith anchors

[1] Generalized Global Symmetries 2015 · arXiv:1412.5148
[2] 205, American Mathematical Society, Providence, RI, 2015,MR3242743 DOI:10.1090/surv/205 2015 · doi:10.1090/surv/205
[3] Kramers-Wannier duality from conformal defects 2004 · arXiv:cond-mat/0404051
[4] Topological defects for the free boson CFT 2007 · arXiv:0705.3129
[5] Defect lines, dualities, and generalised orbifolds,

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arxiv: 2305.18296 · arxiv_version: 2305.18296v2 · doi: 10.48550/arxiv.2305.18296 · pith_short_12: OWYAY52XYP5Z · pith_short_16: OWYAY52XYP5ZLZN2 · pith_short_8: OWYAY52X
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Canonical record JSON
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