Circling in on correlation functions in π©=2 orbifold theories
Abstract
We review the harmonic superspace formalism for 4d π©=2 theories and apply it to orbifolds of π©=4 Super-Yang-Mills (SYM) theory. These theories have a remarkably similar description to π©=4 SYM, but their planar supergraphs feature topological twist lines which generate phases when intersecting bifundamental hypermultiplet propagators. These cause twisted sector BPS correlators to depend on the coupling g. Twisted Coulomb-branch operators of length L receive a leading perturbative contribution to their two-point function at order πͺ(g2L) from a supergraph involving a wrapped hypermultiplet circle. After performing the complete D-algebra, we show that the supergraph reduces to the universal conformal period WL=binom2LLΞΆ(2Lβ1). We extend this analysis to multiple nested hypermultiplet circles and show that they reproduce a series of higher-order terms in the exact localisation result. A subsequent evaluation of leading contributions to BPS three-point correlators again shows complete agreement with localisation results in extremal case and generates new perturbative data in the non-extremal case. The latter involves one untwisted BPS descendant, which contains physical hypermultiplet fields and can therefore connect directly to the twist-dependent hypermultiplet circle. This reduces the suppression in g, resulting in a contribution 4 g2(β+1) Wβ+1 controlled by a bridge length β rather than by an external operator length Lβ₯β. These examples demonstrate the feasibility of harmonic superspace calculations in orbifold theories and point to various future applications in the context of non-BPS correlators, integrability and marginal deformations.
Related
- Exact three-point functions in π© = 2 superconformal field theories: integrability vs. localization
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- Tensor Decomposition for Energy-Momentum Correlation Functions
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BibTeX
@misc{plat2026circling,
title = {{Circling in on correlation functions in $\mathcalN=2$ orbifold theories}},
author = {Dennis le Plat and Torben Skrzypek},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.28733},
eprint = {2610.28733},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.28733},
}
RIS
TY - UNPB
TI - Circling in on correlation functions in π©=2 orbifold theories
AU - Dennis le Plat
AU - Torben Skrzypek
PY - 2026
DA - 2026/10/20
PB - arXiv
DO - 10.48550/arxiv.2610.28733
UR - https://arxiv.org/abs/2610.28733
AB - We review the harmonic superspace formalism for 4d π©=2 theories and apply it to orbifolds of π©=4 Super-Yang-Mills (SYM) theory. These theories have a remarkably similar description to π©=4 SYM, but their planar supergraphs feature topological twist lines which generate phases when intersecting bifundamental hypermultiplet propagators. These cause twisted sector BPS correlators to depend on the coupling g. Twisted Coulomb-branch operators of length L receive a leading perturbative contribution to their two-point function at order πͺ(g^2L) from a supergraph involving a wrapped hypermultiplet circle. After performing the complete D-algebra, we show that the supergraph reduces to the universal conformal period W_L=binom2LLΞΆ(2Lβ1). We extend this analysis to multiple nested hypermultiplet circles and show that they reproduce a series of higher-order terms in the exact localisation result. A subsequent evaluation of leading contributions to BPS three-point correlators again shows complete agreement with localisation results in extremal case and generates new perturbative data in the non-extremal case. The latter involves one untwisted BPS descendant, which contains physical hypermultiplet fields and can therefore connect directly to the twist-dependent hypermultiplet circle. This reduces the suppression in g, resulting in a contribution 4 g^2(β+1) W_β+1 controlled by a bridge length β rather than by an external operator length Lβ₯β. These examples demonstrate the feasibility of harmonic superspace calculations in orbifold theories and point to various future applications in the context of non-BPS correlators, integrability and marginal deformations.
ER -