On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decay

Abstract We propose the reaction $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - , with the $$\Sigma ^{*-}$$ Σ ∗ - decaying to $$\pi ^- \Lambda $$ π - Λ in order to show evidence for the existence of two $$\Xi (1820)$$ Ξ ( 1820 ) states, one around 1824...

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Main Authors: Man-Yu Duan, Jing Song, Wei-Hong Liang, E. Oset
Format: Article
Language:English
Published: SpringerOpen 2024-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-024-13293-5
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author Man-Yu Duan
Jing Song
Wei-Hong Liang
E. Oset
author_facet Man-Yu Duan
Jing Song
Wei-Hong Liang
E. Oset
author_sort Man-Yu Duan
collection DOAJ
description Abstract We propose the reaction $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - , with the $$\Sigma ^{*-}$$ Σ ∗ - decaying to $$\pi ^- \Lambda $$ π - Λ in order to show evidence for the existence of two $$\Xi (1820)$$ Ξ ( 1820 ) states, one around 1824 MeV and narrow, and another one around 1875 MeV and wide. The phase space for $$\bar{K}^0 \Sigma ^{*-}$$ K ¯ 0 Σ ∗ - production reduces the effect of the lower mass resonance, magnifying the effect of the higher mass resonance that shows clearly over the phase space. The estimated rate of the production is bigger than the one of the $$\psi (3686) \rightarrow \bar{\Xi }^+ K^- \Lambda $$ ψ ( 3686 ) → Ξ ¯ + K - Λ reaction, where a clear peak for $$\Xi (1820)$$ Ξ ( 1820 ) was observed by the BESIII collaboration, what makes the Beijing facility ideal to carry out the reaction proposed.
format Article
id doaj-art-7f3cddf0a472480faff824d67f4e9d17
institution Kabale University
issn 1434-6052
language English
publishDate 2024-09-01
publisher SpringerOpen
record_format Article
series European Physical Journal C: Particles and Fields
spelling doaj-art-7f3cddf0a472480faff824d67f4e9d172024-11-17T12:45:24ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522024-09-018491510.1140/epjc/s10052-024-13293-5On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decayMan-Yu Duan0Jing Song1Wei-Hong Liang2E. Oset3Departamento de Física Teórica and IFIC, Centro Mixto Universidad de Valencia-CSIC Institutos de Investigación de PaternaSchool of Physics, Southeast UniversityDepartment of Physics, Guangxi Normal UniversitySchool of Physics, Southeast UniversityAbstract We propose the reaction $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - , with the $$\Sigma ^{*-}$$ Σ ∗ - decaying to $$\pi ^- \Lambda $$ π - Λ in order to show evidence for the existence of two $$\Xi (1820)$$ Ξ ( 1820 ) states, one around 1824 MeV and narrow, and another one around 1875 MeV and wide. The phase space for $$\bar{K}^0 \Sigma ^{*-}$$ K ¯ 0 Σ ∗ - production reduces the effect of the lower mass resonance, magnifying the effect of the higher mass resonance that shows clearly over the phase space. The estimated rate of the production is bigger than the one of the $$\psi (3686) \rightarrow \bar{\Xi }^+ K^- \Lambda $$ ψ ( 3686 ) → Ξ ¯ + K - Λ reaction, where a clear peak for $$\Xi (1820)$$ Ξ ( 1820 ) was observed by the BESIII collaboration, what makes the Beijing facility ideal to carry out the reaction proposed.https://doi.org/10.1140/epjc/s10052-024-13293-5
spellingShingle Man-Yu Duan
Jing Song
Wei-Hong Liang
E. Oset
On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decay
European Physical Journal C: Particles and Fields
title On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decay
title_full On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decay
title_fullStr On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decay
title_full_unstemmed On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decay
title_short On the search for the two poles of the $$\Xi (1820)$$ Ξ ( 1820 ) in the $$\psi (3686) \rightarrow \bar{\Xi }^+ \bar{K}^0 \Sigma ^{*-}(\pi ^- \Lambda )$$ ψ ( 3686 ) → Ξ ¯ + K ¯ 0 Σ ∗ - ( π - Λ ) decay
title_sort on the search for the two poles of the xi 1820 ξ 1820 in the psi 3686 rightarrow bar xi bar k 0 sigma pi lambda ψ 3686 ξ ¯ k ¯ 0 σ ∗ π λ decay
url https://doi.org/10.1140/epjc/s10052-024-13293-5
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