Abstract

Precision phenomenology at the LHC requires accounting for both higher-order QCD and electroweak corrections as well as for photon-initiated subprocesses. Building upon the recent NNPDF3.1 fit, in this work the photon content of the proton is determined within a global analysis supplemented by the LUXqed constraint relating the photon PDF to lepton-proton scattering structure functions: NNPDF3.1luxQED. The uncertainties on the resulting photon PDF are at the level of a few percent, with photons carrying up to \simeq0.5\%≃0.5% of the proton’s momentum. We study the phenomenological implications of NNPDF3.1luxQED at the LHC for Drell-Yan, vector boson pair, top quark pair, and Higgs plus vector boson production. We find that photon-initiated contributions can be significant for many processes, leading to corrections of up to 20\%20%. Our results represent a state-of-the-art determination of the partonic structure of the proton including its photon component.

Highlights

  • We find that photon-initiated corrections computed with NNPDF3.1luxQED can be significant for many processes, leading to corrections of up to 20% depending on the kinematics

  • Parton distributions with QED effects and a photon parton distribution functions (PDFs) are an essential component in highprecision calculations of many LHC processes

  • |y | h driven strategy to determine the photon PDF, independently parametrising γ(x, Q0) and fitting it using constraints from Drell-Yan measurements at the LHC. While this strategy minimised the theoretical bias due to model assumptions, the lack of a precise experimental handle to constrain the photon PDF led to large uncertainties

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Summary

Introduction

Recent progress in the computation of higher-order QCD corrections to LHC processes is such that the current state-of-the-art accuracy is NNLO, with even N3LO calculations available in some relevant cases (see Ref. [1] for a review). The photon PDF is parametrised in a model-independent way using an artificial neural network and constrained by LHC Drell-Yan measurements This procedure was adopted in the NNPDF2.3/3.0QED determinations [23, 37,38,39]. Building upon the recent NNPDF3.1 fit [16], the goal of this paper is to perform a global PDF analysis including QED corrections where the LUXqed calculation is used to constrain the photon PDF. The resulting PDF set, NNPDF3.1luxQED, represents a state-of-the-art determination of the partonic content of the proton including its photon component. We find that photon-initiated corrections computed with NNPDF3.1luxQED can be significant for many processes, leading to corrections of up to 20% depending on the kinematics These PI contributions are consistent with previous estimates based on NNPDF3.0QED within uncertainties in the kinematic region Q >∼ MZ , with larger differences in processes for which Q < MZ. The full breakdown of the χ2/Ndat values in NNPDF3.1luxQED and its comparison with those in NNPDF3.1 is collected in Appendix A

Fit settings
Experimental data
The LUXqed formalism
Theoretical calculations
Fitting strategy
The uncertainties on the photon PDF
The photon PDF
QED effects on the quark and gluon PDFs
Partonic luminosities
The momentum fraction carried by photons
Photon-initiated processes at the LHC
Drell-Yan production
Findings
Summary
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