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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...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2002
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0550-3213(03)00035-X http://cds.cern.ch/record/589274 |
_version_ | 1780899629561282560 |
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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 |
record_format | invenio |
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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