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N=2 coset compactifications with nondiagonal invariants

TLDR
In this paper, the authors consider four-dimensional string models obtained by tensoring N = 2 coset theories with noniagonal modular invariants and present results from a systematic analysis including moddings by discrete symmetries.
Abstract
We consider four-dimensional string models obtained by tensoring N=2 coset theories with nondiagonal modular invariants. We present results from a systematic analysis including moddings by discrete symmetries.

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Symmetries and strings of adjoint QCD2

TL;DR: In this paper, the symmetries of massless two-dimensional adjoint QCD with gauge group SU(N) were revisited and it was shown that the theory in fact admits ∼ 22N non-invertible symmets which severely constrain the possible infrared phases and massive excitations.
Journal ArticleDOI

Symmetries and Strings of Adjoint QCD${}_2$

TL;DR: In this paper, the symmetries of massless two-dimensional adjoint QCD with gauge group $SU(N) were revisited and it was shown that the theory in fact admits non-invertible symmetry which severely constrain the possible infrared phases and massive excitations.
Journal ArticleDOI

Implications of an arithmetical symmetry of the commutant for modular invariants

TL;DR: In this article, the existence of an arithmetical symmetry for the commutant of the modular matrices S and T was shown to hold for all affine simple Lie algebras at all levels.
Journal ArticleDOI

From conformal embeddings to quantum symmetries: an exceptional SU(4) example

TL;DR: In this paper, the authors discuss algebraic tools that are used to describe the quantum symmetries of Boundary Conformal Field Theories on a torus and illustrate these notions with the example of the conformal embedding of SU(4 at level 4 into Spin(15) at level 1, leading to the exceptional quantum graph 4(SU(4)), and determine its algebra of quantum symmetry.
Journal ArticleDOI

Chiral primaries in strange metals

TL;DR: In this article, it was shown that the coset chiral algebra of the low energy theory decomposes into a finite number of sectors which are parametrized by special necklaces.
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