Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalism
Abstract We study the S-wave $$D\varXi $$ DΞ bound state in the Bethe–Salpeter formalism in the ladder and instantaneous approximations. With the kernel generated by the hadronic effective Lagrangian, two open-charmed bound states, which quantum numbers are $$I=0$$ I=0 , $$J^P=(\frac{1}{2})^-$$ JP=(...
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2018-05-01
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Series: | European Physical Journal C: Particles and Fields |
Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-018-5874-1 |
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doaj-e714efb1aa754c30ab29c7dbe9c71abb2020-11-24T22:17:20ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-05-017851810.1140/epjc/s10052-018-5874-1Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalismChao Wang0Liang-Liang Liu1Xian-Wei Kang2Xin-Heng Guo3Rui-Wu Wang4Center for Ecological and Environmental Sciences, Key Laboratory for Space Bioscience and Biotechnology, Northwestern Polytechnical UniversityCollege of Physics and Information Engineering, Shanxi Normal UniversityCollege of Nuclear Science and Technology, Beijing Normal UniversityCollege of Nuclear Science and Technology, Beijing Normal UniversityCenter for Ecological and Environmental Sciences, Key Laboratory for Space Bioscience and Biotechnology, Northwestern Polytechnical UniversityAbstract We study the S-wave $$D\varXi $$ DΞ bound state in the Bethe–Salpeter formalism in the ladder and instantaneous approximations. With the kernel generated by the hadronic effective Lagrangian, two open-charmed bound states, which quantum numbers are $$I=0$$ I=0 , $$J^P=(\frac{1}{2})^-$$ JP=(12)- and $$I=1$$ I=1 , $$J^P=(\frac{1}{2})^-$$ JP=(12)- , respectively, are predicted as new candidates of hadronic pentaquark molecules in our formalism. If existing, they could contribute to the broad 3188 MeV structure near the five new narrow $$\varOmega _c$$ Ωc states observed recently by the LHCb Collaboration.http://link.springer.com/article/10.1140/epjc/s10052-018-5874-1 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Chao Wang Liang-Liang Liu Xian-Wei Kang Xin-Heng Guo Rui-Wu Wang |
spellingShingle |
Chao Wang Liang-Liang Liu Xian-Wei Kang Xin-Heng Guo Rui-Wu Wang Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalism European Physical Journal C: Particles and Fields |
author_facet |
Chao Wang Liang-Liang Liu Xian-Wei Kang Xin-Heng Guo Rui-Wu Wang |
author_sort |
Chao Wang |
title |
Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalism |
title_short |
Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalism |
title_full |
Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalism |
title_fullStr |
Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalism |
title_full_unstemmed |
Possible open-charmed pentaquark molecule $$\varOmega _c(3188)$$ Ωc(3188) – the $$D \varXi $$ DΞ bound state – in the Bethe–Salpeter formalism |
title_sort |
possible open-charmed pentaquark molecule $$\varomega _c(3188)$$ ωc(3188) – the $$d \varxi $$ dξ bound state – in the bethe–salpeter formalism |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2018-05-01 |
description |
Abstract We study the S-wave $$D\varXi $$ DΞ bound state in the Bethe–Salpeter formalism in the ladder and instantaneous approximations. With the kernel generated by the hadronic effective Lagrangian, two open-charmed bound states, which quantum numbers are $$I=0$$ I=0 , $$J^P=(\frac{1}{2})^-$$ JP=(12)- and $$I=1$$ I=1 , $$J^P=(\frac{1}{2})^-$$ JP=(12)- , respectively, are predicted as new candidates of hadronic pentaquark molecules in our formalism. If existing, they could contribute to the broad 3188 MeV structure near the five new narrow $$\varOmega _c$$ Ωc states observed recently by the LHCb Collaboration. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-018-5874-1 |
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