The ADE quantum field theory algebra and symplectic reflection algebra conjecture

Let XX be a resolution of an ADE singularity, with deformation Oϵ,λ1,,λr(X)\mathscr O_{\epsilon,\lambda_1,\dots,\lambda_r}(X) of its algebra of functions, where rr is the ADE rank, and let UδQFT(Oϵ,λ1,,λr(X)glN)U^{QFT}_\delta(\mathscr O_{\epsilon,\lambda_1,\dots,\lambda_r}(X)\otimes\mathfrak{gl}_N) be the deformation obtained from the five-dimensional quantum field theory. Let KK be the charge of framed torsion-free sheaves. ADE large-charge conjecture. The algebra UδQFT(Oϵ,λ1,,λr(X)glN)U^{QFT}_\delta(\mathscr O_{\epsilon,\lambda_1,\dots,\lambda_r}(X)\otimes\mathfrak{gl}_N) is the large-KK limit of a deformation quantization of the moduli of framed torsion-free sheaves of charge KK and rank NN on the noncommutative deformation of XX. For N=1N=1, it should be the large-KK limit of the symplectic reflection algebra for the wreath-product action SKΓKS_K\ltimes\Gamma^K on C2K\mathbb C^{2K}, where ΓSU(2)\Gamma\subset SU(2) is the finite subgroup associated to the ADE singularity. This conjecture proposes an algebraic realization of the five-dimensional theory through moduli-space quantizations; proving it requires constructing and identifying the relevant large-charge limits.

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Primary source

Kevin Costello, “Holography and Koszul duality: the example of the M2 brane”, arXiv:1705.02500 (2017).

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