CHY-Graphs on a Torus
Carlos Cardona, Humberto Gomez
TL;DR
The paper advances CHY methods to one-loop by formulating a torus-based (genus-1) construction on the moduli space ${\mathfrak M}_{1,n}$ using new connectors $H_{a:a}, T_{a:b}, G^{\pm}_{a:b}$. It provides a concrete, graphical, and rule-based translation between tree-level CHY integrands on ${\mathfrak M}_{0,n}$ and one-loop CHY integrands on ${\mathfrak M}_{1,n}$, with explicit application to bi-adjoint $\Phi^3$ theory and both forward- and inverse-constructions that map to and from one-loop Feynman diagrams. Central results include a proposition constraining valid one-loop integrands to products of chains with a fixed line/anti-line balance, and a construction rule that replaces sphere connectors with torus connectors while preserving loop topology. The Lambda-algorithm is employed to evaluate the resulting CHY graphs, yielding known one-loop topologies such as triangles and boxes, and clarifying the relationship between CHY integrands and standard Feynman diagrams. The work also discusses tadpole absence, potential higher-loop extensions, and a graphical blueprint for extending CHY to broader theories with loop-level CHY descriptions.
Abstract
Recently, we proposed a new approach using a punctured Elliptic curve in the CHY framework in order to compute one-loop scattering amplitudes. In this note, we further develop this approach by introducing a set of connectors, which become the main ingredient to build integrands on $\mathfrak{M}_{1,n}$, the moduli space of n-punctured Elliptic curves. As a particular application, we study the $Φ^3$ bi-adjoint scalar theory. We propose a set of rules to construct integrands on $\mathfrak{M}_{1,n}$ from $Φ^ 3$ integrands on $\mathfrak{M}_{0,n}$, the moduli space of n-punctured spheres. We illustrate these rules by computing a variety of $Φ^3$ one-loop Feynman diagrams. Conversely, we also provide another set of rules to compute the corresponding CHY-integrand on $\mathfrak{M}_{1,n}$ by starting instead from a given $Φ^ 3$ one-loop Feynman diagram. In addition, our results can easily be extended to higher loops.
