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The Photon Content of the Proton

The photon PDF of the proton is needed for precision comparisons of LHC cross sections with theoretical predictions. In a recent paper, we showed how the photon PDF could be determined in terms of the electromagnetic proton structure functions F$_{2}$ and F$_{L}$ measured in electron-proton scatteri...

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Autores principales: Manohar, Aneesh V., Nason, Paolo, Salam, Gavin P., Zanderighi, Giulia
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP12(2017)046
http://cds.cern.ch/record/2291604
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author Manohar, Aneesh V.
Nason, Paolo
Salam, Gavin P.
Zanderighi, Giulia
author_facet Manohar, Aneesh V.
Nason, Paolo
Salam, Gavin P.
Zanderighi, Giulia
author_sort Manohar, Aneesh V.
collection CERN
description The photon PDF of the proton is needed for precision comparisons of LHC cross sections with theoretical predictions. In a recent paper, we showed how the photon PDF could be determined in terms of the electromagnetic proton structure functions F$_{2}$ and F$_{L}$ measured in electron-proton scattering experiments, and gave an explicit formula for the PDF including all terms up to next-to-leading order. In this paper we give details of the derivation. We obtain the photon PDF using the factorisation theorem and applying it to suitable BSM hard scattering processes. We also obtain the same PDF in a process-independent manner using the usual definition of PDFs in terms of light-cone Fourier transforms of products of operators. We show how our method gives an exact representation for the photon PDF in terms of F$_{2}$ and F$_{L}$ , valid to all orders in QED and QCD, and including all non-perturbative corrections. This representation is then used to give an explicit formula for the photon PDF to one order higher than our previous result. We also generalise our results to obtain formulæ for the polarised photon PDF, as well as the photon TMDPDF. Using our formula, we derive the P$_{γi}$ subset of DGLAP splitting functions to order αα$_{s}$ and α$^{2}$, which agree with known results. We give a detailed explanation of the approach that we follow to determine a photon PDF and its uncertainty within the above framework.
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spelling cern-22916042021-11-13T12:51:33Zdoi:10.1007/JHEP12(2017)046http://cds.cern.ch/record/2291604engManohar, Aneesh V.Nason, PaoloSalam, Gavin P.Zanderighi, GiuliaThe Photon Content of the Protonhep-phParticle Physics - PhenomenologyThe photon PDF of the proton is needed for precision comparisons of LHC cross sections with theoretical predictions. In a recent paper, we showed how the photon PDF could be determined in terms of the electromagnetic proton structure functions F$_{2}$ and F$_{L}$ measured in electron-proton scattering experiments, and gave an explicit formula for the PDF including all terms up to next-to-leading order. In this paper we give details of the derivation. We obtain the photon PDF using the factorisation theorem and applying it to suitable BSM hard scattering processes. We also obtain the same PDF in a process-independent manner using the usual definition of PDFs in terms of light-cone Fourier transforms of products of operators. We show how our method gives an exact representation for the photon PDF in terms of F$_{2}$ and F$_{L}$ , valid to all orders in QED and QCD, and including all non-perturbative corrections. This representation is then used to give an explicit formula for the photon PDF to one order higher than our previous result. We also generalise our results to obtain formulæ for the polarised photon PDF, as well as the photon TMDPDF. Using our formula, we derive the P$_{γi}$ subset of DGLAP splitting functions to order αα$_{s}$ and α$^{2}$, which agree with known results. We give a detailed explanation of the approach that we follow to determine a photon PDF and its uncertainty within the above framework.The photon PDF of the proton is needed for precision comparisons of LHC cross sections with theoretical predictions. In a recent paper, we showed how the photon PDF could be determined in terms of the electromagnetic proton structure functions $F_2$ and $F_L$ measured in electron-proton scattering experiments, and gave an explicit formula for the PDF including all terms up to next-to-leading order. In this paper we give details of the derivation. We obtain the photon PDF using the factorisation theorem and applying it to suitable BSM hard scattering processes. We also obtain the same PDF in a process-independent manner using the usual definition of PDFs in terms of light-cone Fourier transforms of products of operators. We show how our method gives an exact representation for the photon PDF in terms of $F_2$ and $F_L$, valid to all orders in QED and QCD, and including all non-perturbative corrections. This representation is then used to give an explicit formula for the photon PDF to one order higher than our previous result. We also generalise our results to obtain formul\ae\ for the polarised photon PDF, as well as the photon TMDPDF. Using our formula, we derive the $P_{\gamma i}$ subset of DGLAP splitting functions to order $\alpha \alpha_s$ and $\alpha^2$, which agree with known results. We give a detailed explanation of the approach that we follow to determine a photon PDF and its uncertainty within the above framework.arXiv:1708.01256CERN-TH-2017-141oai:cds.cern.ch:22916042017-08-03
spellingShingle hep-ph
Particle Physics - Phenomenology
Manohar, Aneesh V.
Nason, Paolo
Salam, Gavin P.
Zanderighi, Giulia
The Photon Content of the Proton
title The Photon Content of the Proton
title_full The Photon Content of the Proton
title_fullStr The Photon Content of the Proton
title_full_unstemmed The Photon Content of the Proton
title_short The Photon Content of the Proton
title_sort photon content of the proton
topic hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP12(2017)046
http://cds.cern.ch/record/2291604
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