Abstract

We construct a diagrammatic coaction acting on one-loop Feynman graphs and their cuts. The graphs are naturally identified with the corresponding (cut) Feynman integrals in dimensional regularization, whose coefficients of the Laurent expansion in the dimensional regulator are multiple polylogarithms (MPLs). Our main result is the conjecture that this diagrammatic coaction reproduces the combinatorics of the coaction on MPLs order by order in the Laurent expansion. We show that our conjecture holds in a broad range of nontrivial one-loop integrals. We then explore its consequences for the study of discontinuities of Feynman integrals, and the differential equations that they satisfy. In particular, using the diagrammatic coaction along with information from cuts, we explicitly derive differential equations for any one-loop Feynman integral. We also explain how to construct the symbol of any one-loop Feynman integral recursively. Finally, we show that our diagrammatic coaction follows, in the special case of one-loop integrals, from a more general coaction proposed recently, which is constructed by pairing master integrands with corresponding master contours.

Highlights

  • Feynman integrals are central objects in the perturbative approach to quantum field theory

  • Since we have argued that all one-loop Feynman integrals, as well as their cuts, can be expressed in terms of multiple polylogarithms (MPLs), we give a short review of the mathematics of MPLs and their algebraic properties

  • Our main result is the conjecture (4.12), stating that the coaction of eq (4.7), defined purely in terms of graphs, exactly reproduces the combinatorics of the coaction on MPLs when applied to the Laurent coefficients in the expansion of Feynman integrals

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Summary

Introduction

Feynman integrals are central objects in the perturbative approach to quantum field theory. Understanding the mathematics and algebraic structure of MPLs has led both to new efficient techniques to evaluate Feynman integrals [3,4,5,6,7,8,9] and to tools to handle the complicated analytic expressions inherent to these computations [10] It is known, that starting from two loops there are Feynman integrals that cannot be written in terms of MPLs only, and generalizations to elliptic curves appear [11,12,13,14,15,16,17,18,19,20,21,22]. We include several appendices where we summarize the notation and review some mathematical concepts used throughout the paper, and we present explicit results for the (cut) integrals

One-loop Feynman integrals
One-loop cut integrals
Review of multiple polylogarithms
First examples of the diagrammatic representation of the coaction
The massless bubble integral
The triangle integral with three massive external legs
The bubble integral with massive propagators
A coaction on cut graphs
The incidence coaction on cut graphs
The deformed incidence coaction
The main conjecture
Dimensional regularization
The diagrammatic coaction in dimensional regularization
The coaction on a pure function f always takes the form
Diagrammatic coaction on some one-loop Feynman integrals
Reducible one-loop integrals
Cancellation of poles
Infrared divergent integrals
Two-mass-easy and two-mass-hard boxes
Box with massive internal propagator
The coaction and extended dual conformal invariance
Discontinuities and the diagrammatic coaction
The first-entry condition
Differential equations for one-loop integrals
Differential equations of one-loop integrals
Symbols of one-loop integrals
10 Relation to other coactions
10.1 The coaction on MPLs
10.2 The coaction on one-loop integrals
11 Conclusions
A Notation
Full Text
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