Abstract
Abstract
We point out that the moduli spaces of all known 3d
$$ \mathcal{N} $$
N
= 8 and
$$ \mathcal{N} $$
N
= 6 SCFTs, after suitable gaugings of finite symmetry groups, have the form ℂ
4r
/Γ where Γ is a real or complex reflection group depending on whether the theory is
$$ \mathcal{N} $$
N
= 8 or
$$ \mathcal{N} $$
N
= 6, respectively. Real reflection groups are either dihedral groups, Weyl groups, or two sporadic cases H3,4 Since the BLG theories and the maximally supersymmetric Yang-Mills theories correspond to dihedral and Weyl groups, it is strongly suggested that there are two yet-to
be-discovered 3d
$$ \mathcal{N} $$
N
= 8 theories for H3,4. We also show that all known
$$ \mathcal{N} $$
N
= 6 theories correspond to complex reflection groups collectively known as G(k, x, N). Along the way, we demonstrate that two ABJM theories (SU(N)
k
x SU(N)
-k
)/ℤ
N
and (U(N)
k
x U(N)
-k
) /ℤ
k
are actually equivalent.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
Cited by
21 articles.
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