{"title":"The Moore-Tachikawa conjecture via shifted symplectic geometry","authors":"Peter Crooks, Maxence Mayrand","doi":"arxiv-2409.03532","DOIUrl":null,"url":null,"abstract":"We use shifted symplectic geometry to construct the Moore-Tachikawa\ntopological quantum field theories (TQFTs) in a category of Hamiltonian\nschemes. Our new and overarching insight is an algebraic explanation for the\nexistence of these TQFTs, i.e. that their structure comes naturally from three\ningredients: Morita equivalence, as well as multiplication and identity\nbisections in abelian symplectic groupoids. Using this insight, we generalize\nthe Moore-Tachikawa TQFTs in two directions. The first generalization concerns a 1-shifted version of the Weinstein\nsymplectic category $\\mathbf{WS}_1$. Each abelianizable quasi-symplectic\ngroupoid $\\mathcal{G}$ is shown to determine a canonical 2-dimensional TQFT\n$\\eta_{\\mathcal{G}}:\\mathbf{Cob}_2\\longrightarrow\\mathbf{WS}_1$. We recover the\nopen Moore-Tachikawa TQFT and its multiplicative counterpart as special cases. Our second generalization is an affinization process for TQFTs. We first\nenlarge Moore and Tachikawa's category $\\mathbf{MT}$ of holomorphic symplectic\nvarieties with Hamiltonian actions to $\\mathbf{AMT}$, a category of affine\nPoisson schemes with Hamiltonian actions of affine symplectic groupoids. We\nthen show that if $\\mathcal{G} \\rightrightarrows X$ is an affine symplectic\ngroupoid that is abelianizable when restricted to an open subset $U \\subseteq\nX$ statisfying Hartogs' theorem, then $\\mathcal{G}$ determines a TQFT\n$\\eta_{\\mathcal{G}} : \\mathbf{Cob}_2 \\longrightarrow \\mathbf{AMT}$. In more\ndetail, we first devise an affinization process sending 1-shifted Lagrangian\ncorrespondences in $\\mathbf{WS}_1$ to Hamiltonian Poisson schemes in\n$\\mathbf{AMT}$. The TQFT is obtained by composing this affinization process\nwith the TQFT $\\eta_{\\mathcal{G}|_U} : \\mathbf{Cob}_2 \\longrightarrow\n\\mathbf{WS}_1$ of the previous paragraph. Our results are also shown to yield\nnew TQFTs outside of the Moore-Tachikawa setting.","PeriodicalId":501155,"journal":{"name":"arXiv - MATH - Symplectic Geometry","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - MATH - Symplectic Geometry","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.03532","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
We use shifted symplectic geometry to construct the Moore-Tachikawa
topological quantum field theories (TQFTs) in a category of Hamiltonian
schemes. Our new and overarching insight is an algebraic explanation for the
existence of these TQFTs, i.e. that their structure comes naturally from three
ingredients: Morita equivalence, as well as multiplication and identity
bisections in abelian symplectic groupoids. Using this insight, we generalize
the Moore-Tachikawa TQFTs in two directions. The first generalization concerns a 1-shifted version of the Weinstein
symplectic category $\mathbf{WS}_1$. Each abelianizable quasi-symplectic
groupoid $\mathcal{G}$ is shown to determine a canonical 2-dimensional TQFT
$\eta_{\mathcal{G}}:\mathbf{Cob}_2\longrightarrow\mathbf{WS}_1$. We recover the
open Moore-Tachikawa TQFT and its multiplicative counterpart as special cases. Our second generalization is an affinization process for TQFTs. We first
enlarge Moore and Tachikawa's category $\mathbf{MT}$ of holomorphic symplectic
varieties with Hamiltonian actions to $\mathbf{AMT}$, a category of affine
Poisson schemes with Hamiltonian actions of affine symplectic groupoids. We
then show that if $\mathcal{G} \rightrightarrows X$ is an affine symplectic
groupoid that is abelianizable when restricted to an open subset $U \subseteq
X$ statisfying Hartogs' theorem, then $\mathcal{G}$ determines a TQFT
$\eta_{\mathcal{G}} : \mathbf{Cob}_2 \longrightarrow \mathbf{AMT}$. In more
detail, we first devise an affinization process sending 1-shifted Lagrangian
correspondences in $\mathbf{WS}_1$ to Hamiltonian Poisson schemes in
$\mathbf{AMT}$. The TQFT is obtained by composing this affinization process
with the TQFT $\eta_{\mathcal{G}|_U} : \mathbf{Cob}_2 \longrightarrow
\mathbf{WS}_1$ of the previous paragraph. Our results are also shown to yield
new TQFTs outside of the Moore-Tachikawa setting.