Determine the four-dimensional charge map and test the Macdonald specialization

Determine directly in four dimensions whether the charge \(R+r\) in the Macdonald index of the \((A_2,D_{3n-2})\) Argyres–Douglas theories maps to either \(-J_{\bm v^{(1)}}\) or \(-J_{\bm v^{(2)}}\) in the proposed \(R\)-twisted three-dimensional reductions, and prove or refute the resulting Macdonald-index specialization for \(n>2\).

Background

The paper conjectures that the four-dimensional grading R+rR+r is identified with one of two Weyl-related three-dimensional topological charges. This conjecture is supported by the known n=2n=2 Macdonald-index matching and by the uniform charge structure of the proposed three-dimensional theories.

For n>2n>2, the paper has no independent four-dimensional calculation of the charge map. A direct computation of the four-dimensional superconformal index, particularly using proposed N=1\mathcal N=1 Lagrangian descriptions, would test both the charge identification and the predicted refined fermionic character.

References

For n>2, we do not have an independent 4d calculation that determines this charge map. The evidence for extending it to general n is the uniform 3d charge structure described above.

SCFT/VOA correspondence and R-twisted reductions of $(A_2,D_{3n-2})$ Argyres--Douglas theories  (2609.04099 - Yoshida, 3 Sep 2026) in Section 6.2, subsection “Conjectural 4d/3d charge identification”; Section 7, Summary and discussion