BLG theories at low values of Chern-Simons coupling

preprint2012arXivOpen access

Abstract

It was checked in paper [1] by comparing the moduli spaces and superconformal indices that two of the BLG theories (SU(2)1×SU(2)−1)/Z2(SU(2)_{1}\times SU(2)_{-1})/{\mathbb Z}_2 and SU(2)2×SU(2)−2SU(2)_2\times SU(2)_{-2} are dual to U(2)1×U(2)−1U(2)_1\times U(2)_{-1} and U(2)2×U(2)−2U(2)_{2}\times U(2)_{-2} ABJM theories, correspondingly. In this paper we consider the BLG theories SU(2)1×SU(2)−1SU(2)_1\times SU(2)_{-1} and (SU(2)2×SU(2)−2)/Z2(SU(2)_2\times SU(2)_{-2})/{\mathbb Z}_2. These theories were noted in [1] to be a tensor product of two interacting N=8{\mathcal N}=8 SCFT's. In this paper we identify the SCFT's that occur in the product. For both theories one of the sectors is the IR limit of N=8{\mathcal N}=8 SU(2) SYM.

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