Abstract

We investigate how loop-level propagators arise from tree level via a forward-limit procedure in two modern approaches to scattering amplitudes, namely the BCFW recursion relations and the scattering equations formalism. In the first part of the paper, we revisit the BCFW construction of one-loop integrands in momentum space, using a convenient parametrisation of the D-dimensional loop momentum. We work out explicit examples with and without supersymmetry, and discuss the non-planar case in both gauge theory and gravity. In the second part of the paper, we study an alternative approach to one-loop integrands, where these are written as worldsheet formulas based on new one-loop scattering equations. These equations, which are inspired by BCFW, lead to standard Feynman-type propagators, instead of the ‘linear’-type loop-level propagators that first arose from the formalism of ambitwistor strings. We exploit the analogies between the two approaches, and present a proof of an all-multiplicity worldsheet formula using the BCFW recursion.

Highlights

  • Two important modern advances in understanding perturbative scattering amplitudes in quantum field theory have been the BCFW recursion relations and the formalism of the scattering equations

  • D Worldsheet formulas with double-forward limit scattering equations 77

  • Motivated by the loop-level BCFW recursion relation and the connection it suggests between the forward-limit terms and standard Feynman-like propagators, we investigate how local integrand expressions can arise from the worldsheet

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Summary

Introduction

Two important modern advances in understanding perturbative scattering amplitudes in quantum field theory have been the BCFW recursion relations and the formalism of the scattering equations. BCFW recursion that is suited to D-dimensional momentum space, describing the cancellation of spurious poles in simple examples with and without supersymmetry, and in non-planar theories; and (ii) present a new set of one-loop scattering equations that yields standard Feynman-type propagators, as opposed to more unorthodox representations of the loop integrand considered previously This new worldsheet approach is inspired by the BCFW story, but does not exhibit spurious poles in the same way.

BCFW recursion at one loop
Residue argument: planar case
Boundary terms
BCFW examples in maximal super-Yang-Mills
Absence of boundary terms for MHV
BCFW examples in pure Yang-Mills: all-plus
Absence of boundary terms for all-plus integrand
Relation to previous BCFW literature
Recursion with unshifted loop momentum
Recursion for the integrated all-plus amplitude
BCFW recursion for non-planar Yang-Mills and gravity
Single BCFW shift
Multiple BCFW shifts versus non-planar factorisation
Worldsheet formulas for quadratic propagators: planar case
Brief review of one-loop worldsheet formulas
Scattering equations for Feynman propagators
The MHV integrand
Toy models
Four and five particles
Beyond MHV
Proof for the MHV integrand via BCFW recursion
The single cut
Factorisation
Scattering equations and measure
Wordsheet integrand
Worldsheet formulas for quadratic propagators: non-planar case
A The one-loop six-point MHV integrand in maximal super-Yang-Mills
D Worldsheet formulas with double-forward limit scattering equations
Discussion
Full Text
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