English

On differential operators for scalar-scaffolded gluons

High Energy Physics - Theory 2025-12-19 v1

Abstract

Recently, based on the curve-integral formulation for stringy Trϕ3\phi^3 amplitudes, a combinatorial formulation for Yang-Mills amplitudes has been proposed which describes gluons using pairs of scalars and produces the nn-gluon amplitude from simple kinematical shift of stringy Trϕ3\phi^3 amplitudes with 2n2n scalars. It has revealed a variety of new properties and structures even for tree-level gluon amplitudes such as hidden zeros and splits, and in this note we provide another example: we study differential operators acting on Yang-Mills amplitudes with respect to 2n2n-scalar kinematic variables, which convert such scalar-scaffolded gluons into scalars. In particular, we find (n1)(n{-}1)-fold differential operators (using 2n2n-scalar variables) that turn the nn-gluon amplitude into a single planar ϕ3\phi^3 diagram; we then generalize such operators to those that convert nn gluons to mixed amplitudes with rr scalars and nrn{-}r gluons (the latter can be viewed as insertions on ϕ3\phi^3 diagrams). We also show that the number of linearly independent mixed amplitudes with rr scalars and nrn-r gluons is given by the number of ϕ3\phi^3 diagrams, the Catalan number Cr2\mathcal{C}_{r-2}, which can be viewed as a generalization of the ``uniqueness" theorem of gluon amplitudes (with r=0r=0). Finally, our construction leads to a planar version of the universal expansion of Yang-Mills amplitudes into a sum of gauge-invariant prefactors built from nested commutators, each accompanied by an mixed amplitude in the natural basis. This formulation significantly reduces the redundancy present in the original expansion.

Keywords

Cite

@article{arxiv.2512.15882,
  title  = {On differential operators for scalar-scaffolded gluons},
  author = {Jin Dong and Yong-Xiang Su and Dongyu Yang},
  journal= {arXiv preprint arXiv:2512.15882},
  year   = {2025}
}

Comments

31 pages + appendix, 18+2 figures

R2 v1 2026-07-01T08:29:59.938Z