We consider string/M-theory reductions on a compact space 𝑋=𝑋loc∪𝑋∘, where 𝑋loc contains the singular locus and 𝑋∘ is its complement. For the resulting supergravity theories, we construct a suitable symmetry topological field theory (SymTFT) associated with the boundary ∂𝑋loc∐∂𝑋∘. We propose that boundary conditions for different Bogomol’nyi-Prasad-Sommerfield branes wrapping the same boundary cycles must be correlated for the SymTFT to yield an absolute theory consistent with quantum gravity. Using heterotic/M-theory duality, this constraint can be translated into a field-theoretic statement, which restricts the global structure of 𝑑≥7, 𝒩=1 supergravity theories to reproduce precisely the landscape of untwisted toroidal heterotic compactifications. Furthermore, for six-dimensional (2, 0) theories, we utilize a subtle interplay between gauged 0-, 2-, and 4-form symmetries to provide a bottom-up explanation of the correlated boundary conditions in K3 compactifications of type IIB.
Gould, D.S., Lin, L., Sabag, E. (2024). Swampland constraints on the symmetry topological field theory of supergravity. PHYSICAL REVIEW D, 109(12), 126005-1-126005-32 [10.1103/physrevd.109.126005].
Swampland constraints on the symmetry topological field theory of supergravity
Lin, Ling
;
2024
Abstract
We consider string/M-theory reductions on a compact space 𝑋=𝑋loc∪𝑋∘, where 𝑋loc contains the singular locus and 𝑋∘ is its complement. For the resulting supergravity theories, we construct a suitable symmetry topological field theory (SymTFT) associated with the boundary ∂𝑋loc∐∂𝑋∘. We propose that boundary conditions for different Bogomol’nyi-Prasad-Sommerfield branes wrapping the same boundary cycles must be correlated for the SymTFT to yield an absolute theory consistent with quantum gravity. Using heterotic/M-theory duality, this constraint can be translated into a field-theoretic statement, which restricts the global structure of 𝑑≥7, 𝒩=1 supergravity theories to reproduce precisely the landscape of untwisted toroidal heterotic compactifications. Furthermore, for six-dimensional (2, 0) theories, we utilize a subtle interplay between gauged 0-, 2-, and 4-form symmetries to provide a bottom-up explanation of the correlated boundary conditions in K3 compactifications of type IIB.File | Dimensione | Formato | |
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