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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...

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Detalles Bibliográficos
Autores principales: Goldman, T, Wang, Fan, Ping, Jialun, Qing, Di
Lenguaje:eng
Publicado: 2006
Materias:
Acceso en línea:https://dx.doi.org/10.1063/1.2176500
http://cds.cern.ch/record/937588
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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.
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institution Organización Europea para la Investigación Nuclear
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publishDate 2006
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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