Cubic color charge correlator in a proton made of three quarks and a gluon

Abstract
The three point correlation function of color charge densities is evaluated explicitly in light -one gauge for a proton on the light cone. This includes both C-conjugation even and odd contributions. We account for perturbative corrections to the three-quark light -cone wave function due to the emission of an internal gluon which is not required to be soft. We verify the Ward identity as well as the cancellation of UV divergences in the sum of all diagrams so that the correlator is independent of the renormalization scale. It does, however, exhibit the well-known soft and collinear singularities. The expressions derived here provide the C-odd contribution to the initial conditions for high-energy evolution of the dipole scattering amplitude to small x. Finally, we also present a numerical model estimate of the impact parameter dependence of quantum color charge three-point correlations in the proton at moderately small x.
Main Authors
Format
Articles Research article
Published
2022
Series
Subjects
Publication in research information system
Publisher
American Physical Society (APS)
The permanent address of the publication
https://urn.fi/URN:NBN:fi:jyu-202204262402Use this for linking
Review status
Peer reviewed
ISSN
2470-0010
DOI
https://doi.org/10.1103/PhysRevD.105.036007
Language
English
Published in
Physical Review D
Citation
  • Dumitru, A., Mäntysaari, H., & Paatelainen, R. (2022). Cubic color charge correlator in a proton made of three quarks and a gluon. Physical Review D, 105(3), Article 036007. https://doi.org/10.1103/PhysRevD.105.036007
License
CC BY 4.0Open Access
Funder(s)
European Commission
Research Council of Finland
Research Council of Finland
Funding program(s)
RIA Research and Innovation Action, H2020
Research costs of Academy Research Fellow, AoF
Academy Research Fellow, AoF
RIA Research and Innovation Action, H2020
Akatemiatutkijan tutkimuskulut, SA
Akatemiatutkija, SA
European CommissionResearch Council of Finland
Funded by the European Union. Views and opinions expressed are however those of the author(s) only and do not necessarily reflect those of the European Union or the European Education and Culture Executive Agency (EACEA). Neither the European Union nor EACEA can be held responsible for them.
Additional information about funding
A. D. thanks the U.S. Department of Energy, Office of Nuclear Physics, for support via Grant No. DE-SC0002307; and The City University of New York for PSC-CUNY Research Grant No. 64025-00 52. R. P. is supported by the Academy of Finland, Project No. 1322507 and by the European Research Council, Grant No. 725369. H. M. is supported by the Academy of Finland Projects No. 338263 and No. 346567, and by the European Research Council Project No. STRONG-2020 (Grant Agreement No. 824093). The content of this article does not reflect the official opinion of the European Union, and responsibility for the information and views expressed therein lies entirely with the authors. Computing resources from CSC—IT Center for Science in Espoo, Finland, and from the Finnish Grid and Cloud Infrastructure (persistent identifier urn:nbn:fi:research-infras-2016072533) were used in this work.
Copyright© 2022 American Physical Society

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