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Identifying the Universal part of TMDs
We attempt to identify a path layout in the definition of transverse-momentum-dependent T-odd parton distribution functions (TMD)s which combines features of both, initial- and final-state interactions, so that it remains universal despite the fact that the Wilson lines entering such TMDs change the...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2016
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/s00601-016-1068-2 http://cds.cern.ch/record/2121099 |
_version_ | 1780949350969507840 |
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author | Van der Veken, F.F. Stefanis, N.G. |
author_facet | Van der Veken, F.F. Stefanis, N.G. |
author_sort | Van der Veken, F.F. |
collection | CERN |
description | We attempt to identify a path layout in the definition of transverse-momentum-dependent T-odd parton distribution functions (TMD)s which combines features of both, initial- and final-state interactions, so that it remains universal despite the fact that the Wilson lines entering such TMDs change their orientation. The generic structure of the quark correlator for this path layout is calculated. |
id | cern-2121099 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | cern-21210992021-05-03T20:18:37Zdoi:10.1007/s00601-016-1068-2http://cds.cern.ch/record/2121099engVan der Veken, F.F.Stefanis, N.G.Identifying the Universal part of TMDsParticle Physics - PhenomenologyParticle Physics - PhenomenologyWe attempt to identify a path layout in the definition of transverse-momentum-dependent T-odd parton distribution functions (TMD)s which combines features of both, initial- and final-state interactions, so that it remains universal despite the fact that the Wilson lines entering such TMDs change their orientation. The generic structure of the quark correlator for this path layout is calculated.We attempt to identify a path layout in the definition of transverse-momentum-dependent T-odd parton distribution functions (TMD)s which combines features of both, initial- and final-state interactions, so that it remains universal despite the fact that the Wilson lines entering such TMDs change their orientation. The generic structure of the quark correlator for this path layout is calculated.RUB-TPII-02-2015arXiv:1601.03223RUB-TPII-02-2015oai:cds.cern.ch:21210992016-01-13 |
spellingShingle | Particle Physics - Phenomenology Particle Physics - Phenomenology Van der Veken, F.F. Stefanis, N.G. Identifying the Universal part of TMDs |
title | Identifying the Universal part of TMDs |
title_full | Identifying the Universal part of TMDs |
title_fullStr | Identifying the Universal part of TMDs |
title_full_unstemmed | Identifying the Universal part of TMDs |
title_short | Identifying the Universal part of TMDs |
title_sort | identifying the universal part of tmds |
topic | Particle Physics - Phenomenology Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/s00601-016-1068-2 http://cds.cern.ch/record/2121099 |
work_keys_str_mv | AT vandervekenff identifyingtheuniversalpartoftmds AT stefanisng identifyingtheuniversalpartoftmds |