Abstract

In this paper we construct a CHY representation for all tree-level primitive QCD amplitudes. The quarks may be massless or massive. We define a generalised cyclic factor $\hat{C}(w,z)$ and a generalised permutation invariant function $\hat{E}(z,p,\varepsilon)$. The amplitude is then given as a contour integral encircling the solutions of the scattering equations with the product $\hat{C} \hat{E}$ as integrand. Equivalently, it is given as a sum over the inequivalent solutions of the scattering equations, where the summand consists of a Jacobian times the product $\hat{C} \hat{E}$. This representation separates information: The generalised cyclic factor does not depend on the helicities of the external particles, the generalised permutation invariant function does not depend on the ordering of the external particles.

Highlights

  • Ingredients for the gluon amplitudes are the Parke-Taylor factor C(w, z), defining the cyclic order and a permutation invariant function E(z, p, ε), containing the information on the helicities of the external particles

  • This representation separates information: The generalised cyclic factor does not depend on the helicities of the external particles, the generalised permutation invariant function does not depend on the ordering of the external particles

  • Parke-Taylor factor does not depend on the helicities of the external particles, the permutation invariant function does not depend on the ordering of the external particles

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Summary

Tree-level primitive QCD amplitudes

We define words and shuffle algebras and review the various relations among primitive amplitudes. Dyck words are a convenient tool to label amplitudes with several quark-anti-quark pairs. At the end of this section we present a minimal amplitude basis

Basic definitions
Dyck words
The amplitude basis
The scattering equations
The massive case
Normalisation
Definition of C
Definition of E
Proof of the CHY representation Let us set
An example
Conclusions
A Orientation of fermion lines
Full Text
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