, The corresponding magnetic gauge group (at position? := l j ) is abelian in the first four cases and nonabelian in the last two
, ? 1: the identity
, ? ? 3 (µ)I (1,0) : the SU (2) electric-flavour currents
, ? ? 3 (?)I (0,1) : the S U (2) magnetic-flavour currents
, ? ? 5 (µ)I (2,0) : products of two electric currents
, ? ? 5 (?)I (0,2) : products of two magnetic currents
,1) : the energy-momentum tensor multiplet A 2 ,
, The bottom componentQpQ r of an electric-current multiplet is the product of an antifundamental and a fundamental chiral scalar (the F -term condition imposesQ 1 Q 1 +Q 2 Q 2 = 0)
, theory has no mixed marginal (or relevant) chiral operators. All exactly-marginal deformations are purely electric or purely magnetic superpotentials
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