Abstract

The massless QCD Lagrangian is conformally invariant and, as a consequence, so are the tree-level scattering amplitudes. However, the implications of this powerful symmetry at loop level are only beginning to be explored systematically. Even for finite loop amplitudes, the way conformal symmetry manifests itself may be subtle, e.g. in the form of anomalous conformal Ward identities. As they are finite and rational, the one-loop all-plus and single-minus amplitudes are a natural first step towards understanding the conformal properties of Yang-Mills theory at loop level. Remarkably, we find that the one-loop all-plus amplitudes are conformally invariant, whereas the single-minus are not. Moreover, we present a formula for the one-loop all-plus amplitudes where the symmetry is manifest term by term. Surprisingly, each term transforms covariantly under directional dual conformal variations. We prove the formula directly using recursive techniques, and check that it has the correct physical factorisations.

Highlights

  • Divergences forces one to introduce a mass scale, which obscures the conformal symmetry of the Lagrangian

  • We present a formula for the one-loop all-plus amplitudes where the symmetry is manifest term by term

  • One might bypass the fundamental problem of divergences by studying finite loop amplitudes, only to find that the idea of conformal symmetry being broken at loop level only by the dimensionful regulators is naıve

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Summary

Manifestly conformal result for the one-loop all-plus amplitude in QCD

The n-gluon all-plus amplitudes vanish at tree level, and are given by finite and rational functions at one loop [19,20,21]. The single-trace components A(n1,1) are colour ordered, namely they receive contributions only from planar graphs where the cyclic ordering of the external legs is fixed to match that of the generators in the corresponding trace Because of this, they are called planar (partial) amplitudes, and their singularities can occur only in channels of adjacent momenta. The summands Ckmn in our formula (2.6) are individually conformally invariant This implies in a very neat way that the one-loop all-plus amplitude is conformally invariant for any number of external gluons. This is just an artefact of the specific representation we chose, and different choices are possible

Proof of manifest conformal symmetry
Hints for dual conformal symmetry
Analytic structure of the amplitude
Soft limit
Collinear limit
Absence of spurious poles
Proof of the new formula via BCFW recursion
Term at infinity
Proof by induction of the new formula
Conclusion and outlook
Full Text
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