Abstract

Motivated by the observation that 2+2=42+2=4, we consider four-dimensional N=2\mathcal{N}=2 superconformal field theories on S2×ΣS^2\timesΣ, turning on a suitable rigid supergravity background. On the one hand, reduction of a four-dimensional theory T{T} on a Riemann surface ΣΣ leads to a family F[T,Σ]\mathscr{F}[{T}, Σ] of two-dimensional (2,2)(2,2) unitary SCFTs, a two-dimensional analog of the four-dimensional theories of class S\mathscr{S}. On the other hand, reduction on S2S^2 yields a non-unitary two-dimensional CFT C[T]\mathscr{C}[{T}] whose chiral algebra is the same as the one associated to T{T} by the standard SCFT/VOA correspondence. This construction upgrades the vertex operator algebra to a full-fledged two-dimensional CFT. What's more, it leads to a novel 2d/2d correspondence, a "2+2=42+2 = 4" analog of the "4+2=64+2=6" AGT correspondence: the S2S^2 partition function of F[T;Σ]\mathscr{F}[{T}; Σ] is computed by correlation functions of C[T]\mathscr{C}[{T}] on ΣΣ. The elliptic genus of F[T;Σ]\mathscr{F}[{T}; Σ] is instead computed by a topological QFT E[T]\mathscr{E}[T] on ΣΣ. A central question is whether one can give a purely two-dimensional presentation of the family F[T;Σ]\mathscr{F}[{T}; Σ] of (2,2)(2, 2) theories. We propose an algorithm to realize the (2,2)(2, 2) theories as gauged linear sigma models when T{T} is an Argyres-Douglas theory of type (A1,A2k)(A_1, A_{2k}) and ΣΣ an nn-punctured sphere. We perform stringent checks of our conjecture for k=1k=1 and k=2k=2.

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