<p>We study aspects of the AdS/CFT correspondence for <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">N</mi> <mo>=</mo> <mn>4</mn> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{N}=4 \)</EquationSource> </InlineEquation> U(<i>N</i>) super Yang-Mills theory on <i>S</i><sup>3</sup><i>/</i>Γ, where Γ ⊂ SU(2) is a finite subgroup leading to an ADE singularity in the bulk AdS geometry. We show that a large vacuum degeneracy arises from the choice of gauge holonomy on <i>S</i><sup>3</sup><i>/</i>Γ. On the gravity side, we argue that the bulk ADE singularity supports topological degrees of freedom responsible for this degeneracy. We then provide a holographic derivation of a corresponding large vacuum degeneracy for class S theories of type U(<i>N</i>), showing that these topological degrees of freedom admit an effective description in terms of a three-dimensional level-<i>N</i> Chern-Simons theory, whose gauge group G is determined by Γ. Finally, we discuss how the one-form symmetries of the <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">N</mi> <mo>=</mo> <mn>4</mn> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{N}=4 \)</EquationSource> </InlineEquation> super Yang-Mills theory are realized on the Chern-Simons theory side.</p>

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On holography with ADE singularities

  • Sunjin Choi,
  • Yuji Tachikawa

摘要

We study aspects of the AdS/CFT correspondence for N = 4 \( \mathcal{N}=4 \) U(N) super Yang-Mills theory on S3/Γ, where Γ ⊂ SU(2) is a finite subgroup leading to an ADE singularity in the bulk AdS geometry. We show that a large vacuum degeneracy arises from the choice of gauge holonomy on S3/Γ. On the gravity side, we argue that the bulk ADE singularity supports topological degrees of freedom responsible for this degeneracy. We then provide a holographic derivation of a corresponding large vacuum degeneracy for class S theories of type U(N), showing that these topological degrees of freedom admit an effective description in terms of a three-dimensional level-N Chern-Simons theory, whose gauge group G is determined by Γ. Finally, we discuss how the one-form symmetries of the N = 4 \( \mathcal{N}=4 \) super Yang-Mills theory are realized on the Chern-Simons theory side.