Addendum: Measurement and QCD analysis of double-differential inclusive jet cross sections in proton-proton collisions at √s=13 TeV

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dc.authoridMartinez Rivero, Celso/0000-0002-3224-956X
dc.authoridPerez-Calero Yzquierdo, Antonio/0000-0003-3036-7965
dc.authoridDella Ricca, Giuseppe/0000-0003-2831-6982
dc.authoridBelyaev, Andrey/0000-0003-1692-1173
dc.authoridCalderon, Dr. Alicia/0000-0002-7205-2040
dc.authoridVenditti, Rosamaria/0000-0001-6925-8649
dc.authoridPesaresi, Mark/0000-0002-9759-1083
dc.contributor.authorTumasyan, A.
dc.contributor.authorAdam, W.
dc.contributor.authorAndrejkovic, J. W.
dc.contributor.authorBergauer, T.
dc.contributor.authorChatterjee, S.
dc.contributor.authorDragicevic, M.
dc.contributor.authorDel Valle, A. Escalante
dc.date.accessioned2025-03-23T19:44:55Z
dc.date.available2025-03-23T19:44:55Z
dc.date.issued2022
dc.departmentSinop Üniversitesi
dc.description.abstractThe QCD analysis at NNLO is repeated by using the NNLO interpolation grids for the double-differential inclusive jet cross section [1], which were released after the journal publication of the original analysis. The NNLOJET calculation used to derive these grids is based on the leading-colour and leading-flavour-number approximation and does not include the most recent subleading colour contributions. However, these contributions were reported in ref. [2] to be very small in inclusive jet production, in particular for a jet size of R = 0.7. The grids also contain an estimate of the numerical integration uncertainty of around 1% or less. To account for point-to-point fluctuations, this uncertainty, after consultation with the authors of NNLOJET, has been increased by a factor of two; however, its impact in the fit is negligible. A comparison of the measurement with predictions using various PDFs is shown in figure 1. Although the PDF parametrisation remains identical, higher precision in PDF and QCD parameters is expected by using NNLO grids consistently in the QCD analysis. These new results supersede those obtained by using the k-factor technique.
dc.identifier.doi10.1007/JHEP12(2022)035
dc.identifier.issn1029-8479
dc.identifier.issue12
dc.identifier.scopusqualityQ1
dc.identifier.urihttps://doi.org/10.1007/JHEP12(2022)035
dc.identifier.urihttps://hdl.handle.net/11486/7027
dc.identifier.wosWOS:001024176900002
dc.identifier.wosqualityQ1
dc.indekslendigikaynakWeb of Science
dc.language.isoen
dc.publisherSpringer
dc.relation.ispartofJournal of High Energy Physics
dc.relation.publicationcategoryDiğer
dc.rightsinfo:eu-repo/semantics/openAccess
dc.snmzKA_WOS_20250323
dc.titleAddendum: Measurement and QCD analysis of double-differential inclusive jet cross sections in proton-proton collisions at √s=13 TeV
dc.typeCorrection

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