$$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecule

Abstract The analyses of the LHCb data on X(2900) in the $$D^- K^+$$ D - K + spectrum are performed. Both dynamically generated and explicitly introduced $$X_1(2900)$$ X 1 ( 2900 ) are considered. The results show that both these two approaches support the interpretation of $$X_1(2900)$$ X 1 ( 2900...

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Main Authors: Hao Chen, Hong-Rong Qi, Han-Qing Zheng
Format: Article
Language:English
Published: SpringerOpen 2021-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-021-09603-w
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spelling doaj-5fab856b19694c6aa7f5c9ea10e5dc4a2021-09-19T11:18:19ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-09-0181911110.1140/epjc/s10052-021-09603-w$$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K moleculeHao Chen0Hong-Rong Qi1Han-Qing Zheng2Department of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityDepartment of Engineering Physics, Tsinghua UniversityCollege of Physics, Sichuan UniversityAbstract The analyses of the LHCb data on X(2900) in the $$D^- K^+$$ D - K + spectrum are performed. Both dynamically generated and explicitly introduced $$X_1(2900)$$ X 1 ( 2900 ) are considered. The results show that both these two approaches support the interpretation of $$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecular state, with $$J^{P}=1^-$$ J P = 1 - and an iso-singlet interpretation is much more favorable. The effect of triangle singularity on the production of $$X_1(2900)$$ X 1 ( 2900 ) is also discussed, and it is found that it cannot be interpreted as a pure triangle cusp.https://doi.org/10.1140/epjc/s10052-021-09603-w
collection DOAJ
language English
format Article
sources DOAJ
author Hao Chen
Hong-Rong Qi
Han-Qing Zheng
spellingShingle Hao Chen
Hong-Rong Qi
Han-Qing Zheng
$$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecule
European Physical Journal C: Particles and Fields
author_facet Hao Chen
Hong-Rong Qi
Han-Qing Zheng
author_sort Hao Chen
title $$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecule
title_short $$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecule
title_full $$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecule
title_fullStr $$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecule
title_full_unstemmed $$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecule
title_sort $$x_1(2900)$$ x 1 ( 2900 ) as a $$\bar{d}_1 k$$ d ¯ 1 k molecule
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2021-09-01
description Abstract The analyses of the LHCb data on X(2900) in the $$D^- K^+$$ D - K + spectrum are performed. Both dynamically generated and explicitly introduced $$X_1(2900)$$ X 1 ( 2900 ) are considered. The results show that both these two approaches support the interpretation of $$X_1(2900)$$ X 1 ( 2900 ) as a $$\bar{D}_1 K$$ D ¯ 1 K molecular state, with $$J^{P}=1^-$$ J P = 1 - and an iso-singlet interpretation is much more favorable. The effect of triangle singularity on the production of $$X_1(2900)$$ X 1 ( 2900 ) is also discussed, and it is found that it cannot be interpreted as a pure triangle cusp.
url https://doi.org/10.1140/epjc/s10052-021-09603-w
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AT hongrongqi x12900x12900asabard1kd1kmolecule
AT hanqingzheng x12900x12900asabard1kd1kmolecule
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