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PentaQuark Mass and Structure
The Quark Delocalization, Color Screening Model has successfully reproduced the binding energy and structure of 9‐ and 12‐quark systems that are small nuclei, namely 3He and 4He, in a relativistic version. In a non‐relativistic version it has successfully been applied to 6‐quark systems to describe...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2006
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1063/1.2176500 http://cds.cern.ch/record/937588 |
_version_ | 1780909706694361088 |
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author | Goldman, T Wang, Fan Ping, Jialun Qing, Di |
author_facet | Goldman, T Wang, Fan Ping, Jialun Qing, Di |
author_sort | Goldman, T |
collection | CERN |
description | The Quark Delocalization, Color Screening Model has successfully reproduced the binding energy and structure of 9‐ and 12‐quark systems that are small nuclei, namely 3He and 4He, in a relativistic version. In a non‐relativistic version it has successfully been applied to 6‐quark systems to describe baryon‐baryon potentials, phase shifts and cross sections. It is applied here to KN molecular, Jaffe‐Wilczek, Karliner‐Lipkin and tetrahedral structures proposed for the reported pentaquark state, Θ+. In this model, we find that the excitation energy above KN threshold can be reproduced in some cases. The negative parity state is always found at a lower mass than the positive parity one. Concerns regarding additional physics effects which may obviate this result and a conjecture regarding two‐ vs. three‐body final state production of the Θ+ are also noted. |
id | cern-937588 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2006 |
record_format | invenio |
spelling | cern-9375882019-09-30T06:29:59Zdoi:10.1063/1.2176500http://cds.cern.ch/record/937588engGoldman, TWang, FanPing, JialunQing, DiPentaQuark Mass and StructureParticle Physics - PhenomenologyThe Quark Delocalization, Color Screening Model has successfully reproduced the binding energy and structure of 9‐ and 12‐quark systems that are small nuclei, namely 3He and 4He, in a relativistic version. In a non‐relativistic version it has successfully been applied to 6‐quark systems to describe baryon‐baryon potentials, phase shifts and cross sections. It is applied here to KN molecular, Jaffe‐Wilczek, Karliner‐Lipkin and tetrahedral structures proposed for the reported pentaquark state, Θ+. In this model, we find that the excitation energy above KN threshold can be reproduced in some cases. The negative parity state is always found at a lower mass than the positive parity one. Concerns regarding additional physics effects which may obviate this result and a conjecture regarding two‐ vs. three‐body final state production of the Θ+ are also noted.oai:cds.cern.ch:9375882006 |
spellingShingle | Particle Physics - Phenomenology Goldman, T Wang, Fan Ping, Jialun Qing, Di PentaQuark Mass and Structure |
title | PentaQuark Mass and Structure |
title_full | PentaQuark Mass and Structure |
title_fullStr | PentaQuark Mass and Structure |
title_full_unstemmed | PentaQuark Mass and Structure |
title_short | PentaQuark Mass and Structure |
title_sort | pentaquark mass and structure |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1063/1.2176500 http://cds.cern.ch/record/937588 |
work_keys_str_mv | AT goldmant pentaquarkmassandstructure AT wangfan pentaquarkmassandstructure AT pingjialun pentaquarkmassandstructure AT qingdi pentaquarkmassandstructure |