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U_A(1) problems and gluon topology: Anomalous symmetry in QCD

Graham Shore

Hidden Symmetries and Higgs Phenomena. Proceedings,Zuoz 1998, Pages: 201 - 223

Swansea University Author: Graham Shore

Abstract

Many of the distinctive and subtle features of the dynamics in the UA(1) channel in QCD can be related to gluon topology, more precisely to the topological susceptibility χ(k^2) = i \int d^4x e^ikx⟨0|T Q(x) Q(0)|0⟩, where Q = α_s trGμνG ̃μν is the gluon topological charge density. The link is the UA...

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Published in: Hidden Symmetries and Higgs Phenomena. Proceedings,Zuoz 1998
Published: 1998
Online Access: https://arxiv.org/abs/hep-ph/9812354v1
URI: https://cronfa.swan.ac.uk/Record/cronfa32021
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spelling 2017-02-20T22:04:37.4476876 v2 32021 2017-02-20 U_A(1) problems and gluon topology: Anomalous symmetry in QCD 28a24f55687c82d6f3ee378ead3cf234 Graham Shore Graham Shore true false 2017-02-20 FGSEN Many of the distinctive and subtle features of the dynamics in the UA(1) channel in QCD can be related to gluon topology, more precisely to the topological susceptibility χ(k^2) = i \int d^4x e^ikx⟨0|T Q(x) Q(0)|0⟩, where Q = α_s trGμνG ̃μν is the gluon topological charge density. The link is the UA(1) axial (ABJ) anomaly. In this lecture, we describe the anomalous UA(1) chiral Ward identities in a functional formalism and show how two apparently unrelated ‘UA(1) problems’ – the mass of the η′ and the violation of the Ellis- Jaffe sum rule in polarised deep-inelastic scattering – can be explained in terms of the gluon topological susceptibility. They are related through a UA(1) extension of the Goldberger- Treiman formula, which is derived here for QCD with both massless and massive quarks. Book chapter Hidden Symmetries and Higgs Phenomena. Proceedings,Zuoz 1998 201 223 14 12 1998 1998-12-14 https://arxiv.org/abs/hep-ph/9812354v1 COLLEGE NANME Science and Engineering - Faculty COLLEGE CODE FGSEN Swansea University 2017-02-20T22:04:37.4476876 2017-02-20T21:42:42.3291495 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Graham Shore 1
title U_A(1) problems and gluon topology: Anomalous symmetry in QCD
spellingShingle U_A(1) problems and gluon topology: Anomalous symmetry in QCD
Graham Shore
title_short U_A(1) problems and gluon topology: Anomalous symmetry in QCD
title_full U_A(1) problems and gluon topology: Anomalous symmetry in QCD
title_fullStr U_A(1) problems and gluon topology: Anomalous symmetry in QCD
title_full_unstemmed U_A(1) problems and gluon topology: Anomalous symmetry in QCD
title_sort U_A(1) problems and gluon topology: Anomalous symmetry in QCD
author_id_str_mv 28a24f55687c82d6f3ee378ead3cf234
author_id_fullname_str_mv 28a24f55687c82d6f3ee378ead3cf234_***_Graham Shore
author Graham Shore
author2 Graham Shore
format Book chapter
container_title Hidden Symmetries and Higgs Phenomena. Proceedings,Zuoz 1998
container_start_page 201
publishDate 1998
institution Swansea University
college_str Faculty of Science and Engineering
hierarchytype
hierarchy_top_id facultyofscienceandengineering
hierarchy_top_title Faculty of Science and Engineering
hierarchy_parent_id facultyofscienceandengineering
hierarchy_parent_title Faculty of Science and Engineering
department_str School of Biosciences, Geography and Physics - Physics{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Biosciences, Geography and Physics - Physics
url https://arxiv.org/abs/hep-ph/9812354v1
document_store_str 0
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description Many of the distinctive and subtle features of the dynamics in the UA(1) channel in QCD can be related to gluon topology, more precisely to the topological susceptibility χ(k^2) = i \int d^4x e^ikx⟨0|T Q(x) Q(0)|0⟩, where Q = α_s trGμνG ̃μν is the gluon topological charge density. The link is the UA(1) axial (ABJ) anomaly. In this lecture, we describe the anomalous UA(1) chiral Ward identities in a functional formalism and show how two apparently unrelated ‘UA(1) problems’ – the mass of the η′ and the violation of the Ellis- Jaffe sum rule in polarised deep-inelastic scattering – can be explained in terms of the gluon topological susceptibility. They are related through a UA(1) extension of the Goldberger- Treiman formula, which is derived here for QCD with both massless and massive quarks.
published_date 1998-12-14T03:39:10Z
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