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Exact CHY Integrand Construction Using Combinatorial Neural Networks and Discrete Optimization

High Energy Physics - Theory 2026-01-21 v2 Mathematical Physics math.MP

Abstract

Constructing a rational CHY integrand that realizes prescribed physical pole constraints is a discrete inverse problem whose combinatorial complexity grows with multiplicity. We encode the pole hierarchy through generalized pole degrees K(A)K(A) (channels sAs_A), defined as signed internal-edge counts associated with particle subsets in a colored integrand graph. Additivity under integrand multiplication together with the elementary face recursion on the subset lattice expresses all higher-channel K(A)K(A) as linear functions of the two-particle data {K(sij)}\{K(s_{ij})\} and reduces the inverse step to a mixed-integer linear feasibility problem. The subset lattice provides a fixed dependency graph for deterministic message passing with forward evaluation and backward residual propagation; this computation is parameter-free and involves no training. In factorial-rescaled variables K~(A)=(A2)!K(A)\widetilde K(A)=(|A|-2)!\,K(A), every local update is integral, so propagation is exact in the rescaled recursion variables and does not rely on numerical reconstruction. We further organize generalized integrand graphs by an nn-regular grading under multiplication, where degree-zero (0-regular) factors act as M\"obius-invariant insertions that can be decomposed into four-point cross ratios. We illustrate the construction at six and eight points, including pick-pole selection and higher-order pole reduction.

Keywords

Cite

@article{arxiv.2508.02248,
  title  = {Exact CHY Integrand Construction Using Combinatorial Neural Networks and Discrete Optimization},
  author = {Simeng Li and Yaobo Zhang},
  journal= {arXiv preprint arXiv:2508.02248},
  year   = {2026}
}

Comments

73 pages, 44 figures

R2 v1 2026-07-01T04:32:59.963Z