Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons

Detalhes bibliográficos
Autor(a) principal: Osipov, A. A.
Data de Publicação: 2007
Outros Autores: Hiller, B., Blin, A. H., Providência, J. da
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)
Texto Completo: http://hdl.handle.net/10316/4366
https://doi.org/10.1016/j.aop.2006.08.004
Resumo: The combined effective low energy QCD Lagrangians of Nambu-Jona-Lasinio (NJL) and 't Hooft are supplemented with eight-quark interactions. This work is a follow-up of recent findings, namely (i) the six quark flavour determinant 't Hooft term destabilizes the NJL vacuum, (ii) the addition of a chiral invariant eight-fermion contact term renders the ground state of the theory globally stable; (iii) stability constrains the values of coupling constants of the model, meaning that even in the presence of eight-quark forces the system can be unstable in a certain parameter region. In the present work we study a phenomenological output of eight-quark interactions considering the mass spectra of pseudoscalar and scalar mesons. Mixing angles are obtained and their equivalence to the two angle approach is derived. We show that the masses of pseudoscalars are almost neutral to the eight-quark forces. The only marked effect of the second order in the SU(3) breaking is found in the [eta]-[eta]' system. The scalars are more sensitive to the eight-quark interactions. A strong repulsion between the singlet and octet members is the reason for the obtained low mass of the [sigma] state within the model considered.
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spelling Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesonsThe combined effective low energy QCD Lagrangians of Nambu-Jona-Lasinio (NJL) and 't Hooft are supplemented with eight-quark interactions. This work is a follow-up of recent findings, namely (i) the six quark flavour determinant 't Hooft term destabilizes the NJL vacuum, (ii) the addition of a chiral invariant eight-fermion contact term renders the ground state of the theory globally stable; (iii) stability constrains the values of coupling constants of the model, meaning that even in the presence of eight-quark forces the system can be unstable in a certain parameter region. In the present work we study a phenomenological output of eight-quark interactions considering the mass spectra of pseudoscalar and scalar mesons. Mixing angles are obtained and their equivalence to the two angle approach is derived. We show that the masses of pseudoscalars are almost neutral to the eight-quark forces. The only marked effect of the second order in the SU(3) breaking is found in the [eta]-[eta]' system. The scalars are more sensitive to the eight-quark interactions. A strong repulsion between the singlet and octet members is the reason for the obtained low mass of the [sigma] state within the model considered.http://www.sciencedirect.com/science/article/B6WB1-4M27X5C-1/1/d760f5146b5d2572733e496485c4f3052007info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleaplication/PDFhttp://hdl.handle.net/10316/4366http://hdl.handle.net/10316/4366https://doi.org/10.1016/j.aop.2006.08.004engAnnals of Physics. 322:9 (2007) 2021-2054Osipov, A. A.Hiller, B.Blin, A. H.Providência, J. dainfo:eu-repo/semantics/openAccessreponame:Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)instname:Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãoinstacron:RCAAP2022-05-25T03:29:51Zoai:estudogeral.uc.pt:10316/4366Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireopendoar:71602024-03-19T20:59:42.277173Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) - Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãofalse
dc.title.none.fl_str_mv Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
title Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
spellingShingle Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
Osipov, A. A.
title_short Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
title_full Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
title_fullStr Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
title_full_unstemmed Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
title_sort Effects of eight-quark interactions on the hadronic vacuum and mass spectra of light mesons
author Osipov, A. A.
author_facet Osipov, A. A.
Hiller, B.
Blin, A. H.
Providência, J. da
author_role author
author2 Hiller, B.
Blin, A. H.
Providência, J. da
author2_role author
author
author
dc.contributor.author.fl_str_mv Osipov, A. A.
Hiller, B.
Blin, A. H.
Providência, J. da
description The combined effective low energy QCD Lagrangians of Nambu-Jona-Lasinio (NJL) and 't Hooft are supplemented with eight-quark interactions. This work is a follow-up of recent findings, namely (i) the six quark flavour determinant 't Hooft term destabilizes the NJL vacuum, (ii) the addition of a chiral invariant eight-fermion contact term renders the ground state of the theory globally stable; (iii) stability constrains the values of coupling constants of the model, meaning that even in the presence of eight-quark forces the system can be unstable in a certain parameter region. In the present work we study a phenomenological output of eight-quark interactions considering the mass spectra of pseudoscalar and scalar mesons. Mixing angles are obtained and their equivalence to the two angle approach is derived. We show that the masses of pseudoscalars are almost neutral to the eight-quark forces. The only marked effect of the second order in the SU(3) breaking is found in the [eta]-[eta]' system. The scalars are more sensitive to the eight-quark interactions. A strong repulsion between the singlet and octet members is the reason for the obtained low mass of the [sigma] state within the model considered.
publishDate 2007
dc.date.none.fl_str_mv 2007
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dc.identifier.uri.fl_str_mv http://hdl.handle.net/10316/4366
http://hdl.handle.net/10316/4366
https://doi.org/10.1016/j.aop.2006.08.004
url http://hdl.handle.net/10316/4366
https://doi.org/10.1016/j.aop.2006.08.004
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Annals of Physics. 322:9 (2007) 2021-2054
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