Abstract

We construct a family of 4d4d N=1\mathcal{N}=1 theories that we call Eρσ[USp(2N)]E^σ_ρ[USp(2N)] which exhibit a novel type of 4d4d IR duality very reminiscent of the mirror duality enjoyed by the 3d3d N=4\mathcal{N}=4 Tρσ[SU(N)]T^σ_ρ[SU(N)] theories. We obtain the Eρσ[USp(2N)]E^σ_ρ[USp(2N)] theories from the recently introduced E[USp(2N)]E[USp(2N)] theory, by following the RG flow initiated by vevs labelled by partitions ρρ and σσ for two operators transforming in the antisymmetric representations of the USp(2N)×USp(2N)USp(2N) \times USp(2N) IR symmetries of the E[USp(2N)]E[USp(2N)] theory. These vevs are the 4d4d uplift of the ones we turn on for the moment maps of T[SU(N)]T[SU(N)] to trigger the flow to Tρσ[SU(N)]T^σ_ρ[SU(N)]. Indeed the E[USp(2N)]E[USp(2N)] theory, upon dimensional reduction and suitable real mass deformations, reduces to the T[SU(N)]T[SU(N)] theory. In order to study the RG flows triggered by the vevs we develop a new strategy based on the duality webs of the T[SU(N)]T[SU(N)] and E[USp(2N)]E[USp(2N)] theories.

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