J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production
We reassess the decay of the J/ψ into an ω,ϕ,K and one of the f(1370), f(1710), f(1270), f(1525), K(1430) and K(1430) resonances. We benefit from previous works that considered this reaction as a J/ψ decay into three vector mesons, with a scalar or tensor resonance being formed from the interaction...
| Autores: | , , |
|---|---|
| Formato: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2023 |
| País: | España |
| Recursos: | Consejo Superior de Investigaciones Científicas (CSIC) |
| Repositorio: | DIGITAL.CSIC. Repositorio Institucional del CSIC |
| OAI Identifier: | oai:digital.csic.es:10261/358484 |
| Acesso em linha: | http://hdl.handle.net/10261/358484 |
| Access Level: | acceso abierto |
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J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor productionAbreu, L.M.Dai, LianrongOset, EulogiWe reassess the decay of the J/ψ into an ω,ϕ,K and one of the f(1370), f(1710), f(1270), f(1525), K(1430) and K(1430) resonances. We benefit from previous works that considered this reaction as a J/ψ decay into three vector mesons, with a scalar or tensor resonance being formed from the interaction of two of these vectors. The novelty here with respect to former studies is the investigation of the relation between the scalar meson and tensor productions for the first time. To this end, the spin structure of the four vectors present in the production vertex is analyzed, and the D-wave mechanism in the tensor production is included. Then, beyond the ratios studied previously involving scalar states and tensor states independently, new ratios relating the scalar and tensor meson productions are estimated. Our results suggest that the D-wave mechanism of tensor production assumes a relevant contribution. New experimental data reporting the angular distributions of these processes will be important for checking this conclusion.Peer reviewedElsevier BVEuropean CommissionMinisterio de Ciencia e Innovación (España)Generalitat ValencianaAgencia Estatal de Investigación (España)Consejo Superior de Investigaciones Científicas [https://ror.org/02gfc7t72]2024202420232024info:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_6501Publisher's versioninfo:eu-repo/semantics/publishedVersionhttp://hdl.handle.net/10261/358484reponame:DIGITAL.CSIC. Repositorio Institucional del CSICinstname:Consejo Superior de Investigaciones Científicas (CSIC)Inglés#PLACEHOLDER_PARENT_METADATA_VALUE##PLACEHOLDER_PARENT_METADATA_VALUE##PLACEHOLDER_PARENT_METADATA_VALUE#info:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2013-2016/FIS2017-84038-C2-1-Pinfo:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2017-2020/PID2020-112777GB-I00info:eu-repo/grantAgreement/EC/H2020/824093http://dx.doi.org/10.1016/j.physletb.2023.137999Síinfo:eu-repo/semantics/openAccessoai:digital.csic.es:10261/3584842026-05-22T06:33:51Z |
| dc.title.none.fl_str_mv |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production |
| title |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production |
| spellingShingle |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production Abreu, L.M. |
| title_short |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production |
| title_full |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production |
| title_fullStr |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production |
| title_full_unstemmed |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production |
| title_sort |
J/ψ decay to ϕ,ω,K⁎0 plus f0(1370), f0(1710), K0⁎(1430), f2(1270), f2′(1525) and K2⁎(1430): Role of the D-wave for tensor production |
| dc.creator.none.fl_str_mv |
Abreu, L.M. Dai, Lianrong Oset, Eulogi |
| author |
Abreu, L.M. |
| author_facet |
Abreu, L.M. Dai, Lianrong Oset, Eulogi |
| author_role |
author |
| author2 |
Dai, Lianrong Oset, Eulogi |
| author2_role |
author author |
| dc.contributor.none.fl_str_mv |
European Commission Ministerio de Ciencia e Innovación (España) Generalitat Valenciana Agencia Estatal de Investigación (España) Consejo Superior de Investigaciones Científicas [https://ror.org/02gfc7t72] |
| description |
We reassess the decay of the J/ψ into an ω,ϕ,K and one of the f(1370), f(1710), f(1270), f(1525), K(1430) and K(1430) resonances. We benefit from previous works that considered this reaction as a J/ψ decay into three vector mesons, with a scalar or tensor resonance being formed from the interaction of two of these vectors. The novelty here with respect to former studies is the investigation of the relation between the scalar meson and tensor productions for the first time. To this end, the spin structure of the four vectors present in the production vertex is analyzed, and the D-wave mechanism in the tensor production is included. Then, beyond the ratios studied previously involving scalar states and tensor states independently, new ratios relating the scalar and tensor meson productions are estimated. Our results suggest that the D-wave mechanism of tensor production assumes a relevant contribution. New experimental data reporting the angular distributions of these processes will be important for checking this conclusion. |
| publishDate |
2023 |
| dc.date.none.fl_str_mv |
2023 2024 2024 2024 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article http://purl.org/coar/resource_type/c_6501 Publisher's version info:eu-repo/semantics/publishedVersion |
| format |
article |
| status_str |
publishedVersion |
| dc.identifier.none.fl_str_mv |
http://hdl.handle.net/10261/358484 |
| url |
http://hdl.handle.net/10261/358484 |
| dc.language.none.fl_str_mv |
Inglés |
| language_invalid_str_mv |
Inglés |
| dc.relation.none.fl_str_mv |
#PLACEHOLDER_PARENT_METADATA_VALUE# #PLACEHOLDER_PARENT_METADATA_VALUE# #PLACEHOLDER_PARENT_METADATA_VALUE# info:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2013-2016/FIS2017-84038-C2-1-P info:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2017-2020/PID2020-112777GB-I00 info:eu-repo/grantAgreement/EC/H2020/824093 http://dx.doi.org/10.1016/j.physletb.2023.137999 Sí |
| dc.rights.none.fl_str_mv |
info:eu-repo/semantics/openAccess |
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openAccess |
| dc.publisher.none.fl_str_mv |
Elsevier BV |
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Elsevier BV |
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reponame:DIGITAL.CSIC. Repositorio Institucional del CSIC instname:Consejo Superior de Investigaciones Científicas (CSIC) |
| instname_str |
Consejo Superior de Investigaciones Científicas (CSIC) |
| reponame_str |
DIGITAL.CSIC. Repositorio Institucional del CSIC |
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DIGITAL.CSIC. Repositorio Institucional del CSIC |
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15,812429 |