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2d dualities from 4d

by Jiaqun Jiang, Satoshi Nawata, Jiahao Zheng

Submission summary

Authors (as registered SciPost users): Jiang Jiaqun · Satoshi Nawata · Jiahao Zheng
Submission information
Preprint Link: https://arxiv.org/abs/2407.17350v2  (pdf)
Date submitted: 2025-02-17 05:56
Submitted by: Nawata, Satoshi
Submitted to: SciPost Physics
Ontological classification
Academic field: Physics
Specialties:
  • High-Energy Physics - Theory
Approach: Theoretical

Abstract

We find new $\mathcal{N}=(2,2)$ and $\mathcal{N}=(0,2)$ dualities through the twisted compactifications of 4d supersymmetric theories on $S^2$. Our findings include dualities for both $\mathcal{N}=(2,2)$ and $\mathcal{N}=(0,2)$ non-Abelian gauge theories, as well as $\mathcal{N}=(0,2)$ Gauge/Landau-Ginzburg duality.

Author indications on fulfilling journal expectations

  • Provide a novel and synergetic link between different research areas.
  • Open a new pathway in an existing or a new research direction, with clear potential for multi-pronged follow-up work
  • Detail a groundbreaking theoretical/experimental/computational discovery
  • Present a breakthrough on a previously-identified and long-standing research stumbling block

Author comments upon resubmission

First of all, we would like to express our sincere gratitude for the valuable comments provided by the referees. In response to the feedback, we have made major revisions to the manuscript. In the first version, Section 3 focused on the duality of (0,2) SU gauge theories, while Section 4 addressed (0,2) Gauge/Landau-Ginzburg dualities. In the second version, we have combined these two sections into a single, unified section. As a result of further exploration, we have discovered additional new dualities, some of which extend to new trialities. Consequently, the length of the paper has approximately doubled.

List of changes

As noted above, the entire structure of the paper has been reorganized.

Section 2 has undergone a minor revision:
- In Section 2.3, we clarify that the term discussed is the scalar potential, not the superpotential. In an \(\mathcal{N}=(2,2)\) theory, the scalar potential is present even when there is no superpotential.
- Below equation (2.6) for the elliptic genus, we mention that the coordinate ring of the target space \((\mathrak{t} \times \mathrak{t}) / S_N\) is generated by \(\text{Tr}(\phi^i \sigma^j)\). However, we are unclear about the precise relation between these generators, and thus do not fully understand the cancellation mechanism that leads to such a simple expression for the elliptic genus.

Section 3 has undergone a major revision with the addition of new dualities:
- Section 3.1 provides a more detailed discussion of the duality of SU gauge theories originally found by Gadde-Razamat-Willet [arXiv:1506.08795], addressing various subtleties.
- Section 3.2 generalizes the (0,2) Seiberg-like duality for the Sp gauge group into a new triality. In a similar vein, we propose a new triality involving SO gauge theory, SU+1Sym gauge theory, and a Landau-Ginzburg model. Based on these results, we uncover new (0,2) dualities in the following subsections:
- Section 3.3 proposes a new duality between Sp gauge theory and SU quiver gauge theory.
- Section 3.4 presents a duality between two SU+1AS gauge theories.
- Section 3.5 introduces a duality between two SU+1Sym gauge theories.
- Section 3.6 investigates SO and Sp gauge theories with adjoint chiral matter, exploring their dualities with free chiral theories.
- Section 3.7 explores theories that contain both symmetric and anti-symmetric chiral multiplets, presenting a duality to a Landau-Ginzburg model.

We have added Appendix C to provide additional technical details on the (0,2) dualities that are too specialized for the main text:
- Appendix C.1 explains the twisted compactification of the 4d \(\mathcal{N}=1\) Intriligator-Seiberg duality on \(S^2\), which leads to a duality between (0,2) SO gauge theory and a Landau-Ginzburg model.
- Appendix C.2 proposes a triality similar to the one discussed in Section 3.2.
- Appendices C.3 and C.4 cover dualities not included in Section 3.5.

Current status:
In refereeing

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