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The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scattering

We claim that factorization implies that the evolution kernel, defined by the logarithmic derivative of the N-th moment of the structure function d ln F_2^N / d ln Q^2, receives logarithmically enhanced contributions (Sudakov logs) from a single source, namely the constrained invariant mass of the j...

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Detalles Bibliográficos
Autores principales: Gardi, E., Roberts, R.G.
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(03)00035-X
http://cds.cern.ch/record/589274
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author Gardi, E.
Roberts, R.G.
author_facet Gardi, E.
Roberts, R.G.
author_sort Gardi, E.
collection CERN
description We claim that factorization implies that the evolution kernel, defined by the logarithmic derivative of the N-th moment of the structure function d ln F_2^N / d ln Q^2, receives logarithmically enhanced contributions (Sudakov logs) from a single source, namely the constrained invariant mass of the jet. Available results from fixed-order calculations facilitate Sudakov resummation up to the next-to-next-to-leading logarithmic accuracy. We use additional all-order information on the physical kernel from the large-beta_0 limit to model the behaviour of further subleading logs and explore the uncertainty in extracting alpha_s and in determining the magnitude of higher-twist contributions from a comparison with data on high moments.
id cern-589274
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
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spelling cern-5892742023-10-12T05:47:18Zdoi:10.1016/S0550-3213(03)00035-Xhttp://cds.cern.ch/record/589274engGardi, E.Roberts, R.G.The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scatteringParticle Physics - PhenomenologyWe claim that factorization implies that the evolution kernel, defined by the logarithmic derivative of the N-th moment of the structure function d ln F_2^N / d ln Q^2, receives logarithmically enhanced contributions (Sudakov logs) from a single source, namely the constrained invariant mass of the jet. Available results from fixed-order calculations facilitate Sudakov resummation up to the next-to-next-to-leading logarithmic accuracy. We use additional all-order information on the physical kernel from the large-beta_0 limit to model the behaviour of further subleading logs and explore the uncertainty in extracting alpha_s and in determining the magnitude of higher-twist contributions from a comparison with data on high moments.We claim that factorization implies that the evolution kernel, defined by the logarithmic derivative of the N-th moment of the structure function d ln F_2^N / d ln Q^2, receives logarithmically enhanced contributions (Sudakov logs) from a single source, namely the constrained invariant mass of the jet. Available results from fixed-order calculations facilitate Sudakov resummation up to the next-to-next-to-leading logarithmic accuracy. We use additional all-order information on the physical kernel from the large-beta_0 limit to model the behaviour of further subleading logs and explore the uncertainty in extracting alpha_s and in determining the magnitude of higher-twist contributions from a comparison with data on high moments.We claim that factorization implies that the evolution kernel, defined by the logarithmic derivative of the N-th moment of the structure function d ln F_2^N / d ln Q^2, receives logarithmically enhanced contributions (Sudakov logs) from a single source, namely the constrained invariant mass of the jet. Available results from fixed-order calculations facilitate Sudakov resummation up to the next-to-next-to-leading logarithmic accuracy. We use additional all-order information on the physical kernel from the large-beta_0 limit to model the behaviour of further subleading logs and explore the uncertainty in extracting alpha_s and in determining the magnitude of higher-twist contributions from a comparison with data on high moments.We claim that factorization implies that the evolution kernel, defined by the logarithmic derivative of the N th moment of the structure function d ln F 2 N / d ln Q 2 , receives logarithmically enhanced contributions (Sudakov logs) from a single source, namely, the constrained invariant mass of the jet. Available results from fixed-order calculations facilitate Sudakov resummation up to the next-to-next-to-leading logarithmic accuracy. We use additional all-order information on the physical kernel from the large- β 0 limit to model the behaviour of further subleading logs and explore the uncertainty in extracting α s and in determining the magnitude of higher-twist contributions from a comparison with data on high moments.hep-ph/0210429CERN-TH-2002-294CERN-TH-2002-294oai:cds.cern.ch:5892742002-10-30
spellingShingle Particle Physics - Phenomenology
Gardi, E.
Roberts, R.G.
The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scattering
title The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scattering
title_full The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scattering
title_fullStr The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scattering
title_full_unstemmed The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scattering
title_short The interplay between Sudakov resummation, renormalons and higher twist in deep inelastic scattering
title_sort interplay between sudakov resummation, renormalons and higher twist in deep inelastic scattering
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(03)00035-X
http://cds.cern.ch/record/589274
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