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Large N Universality of 4d N=1 SCFTs with Simple Gauge Groups (2510.19136v1)

Published 21 Oct 2025 in hep-th

Abstract: We classify four-dimensional $\mathcal{N}=1$ supersymmetric gauge theories with a simple gauge group admitting a large $N$ limit that flow to non-trivial superconformal fixed points in the infrared. We focus on the cases where the large $N$ limit can be taken while keeping the flavor symmetry fixed so that the putative holographic dual has a fixed gauge group. We find that they can be classified into three types -- Type I, Type II, and Type III -- exhibiting universal behavior. Type I theories have $a \neq c$ in the large $N$ limit and scale linearly in $N$; the gap of scaling dimensions among BPS operators behaves as $1/N$. Type II theories have $a=c$ in the large $N$ limit, and satisfy $a \simeq c \simeq \frac{27}{128} \dim G$, and Type III theories have $a \simeq c \simeq \frac{1}{4} \dim G$. For Type II and Type III theories, the gap of scaling dimensions stays $O(1)$ in the large $N$ limit. We enumerate relevant and marginal operators of these theories and find that non-trivial conformal manifolds emerge upon relevant deformations. Moreover, we find that a modified version of the AdS Weak Gravity Conjecture, based on the supersymmetric Cardy formula, holds for all of these theories, even for finite $N$.

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Open Problems

  1. Existence of IR SCFT for SU(N) with two symmetric pairs and Nf fundamentals
  2. Existence of IR SCFT for SU(N) with mixed symmetric/antisymmetric tensors and chiral matter
  3. Existence of IR SCFT for SU(N) with one symmetric and one antisymmetric pair plus Nf fundamentals
  4. Existence of IR SCFT for SU(N) with one symmetric, two conjugate antisymmetric tensors and chiral matter
  5. Existence of IR SCFT for SU(N) with two symmetrics and two conjugate antisymmetrics plus chiral matter
  6. Existence of IR SCFT for SU(N) with one adjoint and one symmetric pair plus Nf fundamentals
  7. Existence of IR SCFT for SU(N) with one adjoint, one symmetric and one conjugate antisymmetric plus chiral matter
  8. Existence of IR SCFT for SU(N) with one adjoint and one antisymmetric pair plus Nf fundamentals
  9. Existence of IR SCFT for SU(N) with two adjoints plus Nf fundamentals
  10. Existence of IR SCFT for SU(N) Type III theory with one symmetric pair and two antisymmetric pairs plus Nf fundamentals
  11. Existence of IR SCFT for SU(N) Type III theory with three antisymmetric pairs plus Nf fundamentals
  12. Existence of IR SCFT for SU(N) Type III theory with one adjoint and two antisymmetric pairs plus Nf fundamentals
  13. Existence of IR SCFT for SO(N) with one symmetric tensor and Nf vectors
  14. Existence of IR SCFT for SO(N) with one antisymmetric (adjoint) tensor and Nf vectors
  15. Existence of IR SCFT for SO(N) with two symmetric tensors and Nf vectors
  16. Existence of IR SCFT for SO(N) with one symmetric and one antisymmetric tensor plus Nf vectors
  17. Existence of IR SCFT for SO(N) with two antisymmetric tensors and Nf vectors
  18. Existence of IR SCFT for Sp(N) with one symmetric tensor and 2Nf fundamentals
  19. Existence of IR SCFT for Sp(N) with one antisymmetric tensor and 2Nf fundamentals
  20. Existence of IR SCFT for Sp(N) with two symmetric tensors and 2Nf fundamentals
  21. Existence of IR SCFT for Sp(N) with one symmetric and one antisymmetric tensor plus 2Nf fundamentals
  22. Existence of IR SCFT for Sp(N) with two antisymmetric tensors and 2Nf fundamentals (exceptions at small N)
  23. Existence of IR SCFT for Sp(N) Type III theory with two symmetric and one antisymmetric tensor plus 2Nf fundamentals
  24. Existence of IR SCFT for Sp(N) Type III theory with one symmetric and two antisymmetric tensors plus 2Nf fundamentals
  25. Existence of IR SCFT for Sp(N) Type III theory with three antisymmetric tensors and 2Nf fundamentals (exception at N=2, Nf=0)
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