The classical limit geometric Langlands conjecture

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Let CC be the curve, let GG and LG{}^{L}G be a pair of Langlands-dual semisimple groups, and let Higgs⁡\operatorname{\boldsymbol{\mathcal{H}iggs}} and LHiggs⁡{}^{L}\operatorname{\boldsymbol{\mathcal{H}iggs}} denote the corresponding Higgs-bundle moduli stacks. Let Wμ,x\mathbb{W}^{\mu,x} be the classical limit tensorization functors and LHμ,x{}^{L}\mathbb{H}^{\mu,x} the classical limit Hecke functors defined using the classical limit Hecke kernel.

The geometric Langlands correspondence. There exists a canonical equivalence of categories

cl:Dcoh⁡(Higgs⁡,O)⟶≅Dcoh⁡(LHiggs⁡,O),\mathfrak{cl}:D_{\operatorname{coh}}(\operatorname{\boldsymbol{\mathcal{H}iggs}},\mathcal{O})\stackrel{\cong}{\longrightarrow}D_{\operatorname{coh}}({}^{L}\operatorname{\boldsymbol{\mathcal{H}iggs}},\mathcal{O}),

which intertwines the action of the classical limit tensorization functors Wμ,x\mathbb{W}^{\mu,x} with the action of the classical limit Hecke functors LHμ,x{}^{L}\mathbb{H}^{\mu,x}.

This is the proposed classical-limit, or Higgs-bundle, counterpart of the geometric Langlands correspondence. The source motivates it through the classical limit of the constructions, but gives no evidence that the conjecture has been resolved.

References

Primary source

Ron Donagi and Tony Pantev, “Langlands duality for Hitchin systems”, arXiv:math/0604617 (2011).

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