On the singular behavior of the chirality-odd twist-3 parton distribution e(x)

The first moment of the chirality-odd twist-3 parton distribution e(x) is related to the pion-nucleon σ-term, which is important for phenomenology. However, the possible existence of a singular contribution proportional to δ(x) in the distribution prevents the determination of the σ-term with e(x) e...

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Main Authors: J.P. Ma, G.P. Zhang
Format: Article
Language:English
Published: Elsevier 2020-12-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269320307504
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spelling doaj-7e7dfc7a474e4ba0ac63334c9d29a9fd2020-12-09T04:14:37ZengElsevierPhysics Letters B0370-26932020-12-01811135947On the singular behavior of the chirality-odd twist-3 parton distribution e(x)J.P. Ma0G.P. Zhang1CAS Key Laboratory of Theoretical Physics, Institute of Theoretical Physics, Chinese Academy of Sciences, P.O. Box 2735, 100190 Beijing, China; School of Physical Sciences, University of the Chinese Academy of Sciences, 100049 Beijing, China; School of Physics and Center for High-Energy Physics, Peking University, 100871 Beijing, China; Corresponding author.Department of Physics, Yunnan University, Kunming, 650091 Yunnan, ChinaThe first moment of the chirality-odd twist-3 parton distribution e(x) is related to the pion-nucleon σ-term, which is important for phenomenology. However, the possible existence of a singular contribution proportional to δ(x) in the distribution prevents the determination of the σ-term with e(x) extracted from experimental data. There are two approaches to show the existence: the first one is based on an operator identity; the second one is based on a perturbative calculation of a single quark state with finite quark mass. We show that all contributions proportional to δ(x) in the first approach are canceled. For the second approach we find that e(x) of a multiparton state with a massless quark has no contribution with δ(x). Considering that a proton is essentially a multiparton state, the effect of the contribution with δ(x) is expected to be suppressed by light quark masses with arguments from perturbation theory. A detailed discussion of the difference between cut diagrams and uncut diagrams of e(x) is provided.http://www.sciencedirect.com/science/article/pii/S0370269320307504
collection DOAJ
language English
format Article
sources DOAJ
author J.P. Ma
G.P. Zhang
spellingShingle J.P. Ma
G.P. Zhang
On the singular behavior of the chirality-odd twist-3 parton distribution e(x)
Physics Letters B
author_facet J.P. Ma
G.P. Zhang
author_sort J.P. Ma
title On the singular behavior of the chirality-odd twist-3 parton distribution e(x)
title_short On the singular behavior of the chirality-odd twist-3 parton distribution e(x)
title_full On the singular behavior of the chirality-odd twist-3 parton distribution e(x)
title_fullStr On the singular behavior of the chirality-odd twist-3 parton distribution e(x)
title_full_unstemmed On the singular behavior of the chirality-odd twist-3 parton distribution e(x)
title_sort on the singular behavior of the chirality-odd twist-3 parton distribution e(x)
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2020-12-01
description The first moment of the chirality-odd twist-3 parton distribution e(x) is related to the pion-nucleon σ-term, which is important for phenomenology. However, the possible existence of a singular contribution proportional to δ(x) in the distribution prevents the determination of the σ-term with e(x) extracted from experimental data. There are two approaches to show the existence: the first one is based on an operator identity; the second one is based on a perturbative calculation of a single quark state with finite quark mass. We show that all contributions proportional to δ(x) in the first approach are canceled. For the second approach we find that e(x) of a multiparton state with a massless quark has no contribution with δ(x). Considering that a proton is essentially a multiparton state, the effect of the contribution with δ(x) is expected to be suppressed by light quark masses with arguments from perturbation theory. A detailed discussion of the difference between cut diagrams and uncut diagrams of e(x) is provided.
url http://www.sciencedirect.com/science/article/pii/S0370269320307504
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