Schreiber Non-Lagrangian construction of abelian CS/FQH theory

Talks that I will have given:



Abstract: After briefly recalling how the analog of Dirac charge quantization in exotic (effective, higher) gauge theories, providing their global topological completion, is encoded in a choice of classifying space 𝒜\mathscr{A} whose rationalization reflects the flux Bianchi identities, I explain how the choice 𝒜 S 2 P 1 P B U ( 1 ) \mathscr{A} \coloneqq S^2 \simeq \mathbb{C}P^1 \subset \mathbb{C}P^\infty \simeq B \mathrm{U}(1) (“flux quantization in 2-Cohomotopy”) implements effective corrections to ordinary Dirac flux quantization, which over surfaces yields exactly the topological quantum observables of fractional quantum Hall systems, traditionally described by abelian Chern-Simons theory. I close by briefly indicating how this situation is geometrically engineered on probe M5-branes if the M-theory C-field is flux-quantized in 4-Cohomotopy (“Hypothesis H”).


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