The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonances
We perform a theoretical study of the χcJ→ϕK⁎K¯→ϕKπK¯ reaction taking into account the K⁎K¯ final state interaction, which in the chiral unitary approach is responsible, together with its coupled channels, for the formation of the low lying axial vector mesons, in this case the h1(1380) given the se...
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doaj-ee0405b70f5541739066082fe15717a72020-11-25T02:39:33ZengElsevierPhysics Letters B0370-26932019-10-01797The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonancesSheng-Juan Jiang0S. Sakai1Wei-Hong Liang2E. Oset3Department of Physics, Guangxi Normal University, Guilin 541004, China; Guangxi Key Laboratory of Nuclear Physics and Technology, Guangxi Normal University, Guilin 541004, ChinaInstitute of Theoretical Physics, CAS, Zhong Guan Cun East Street 55, 100190 Beijing, ChinaDepartment of Physics, Guangxi Normal University, Guilin 541004, China; Guangxi Key Laboratory of Nuclear Physics and Technology, Guangxi Normal University, Guilin 541004, China; Corresponding author.Departamento de Física Teórica and IFIC, Centro Mixto Universidad de Valencia - CSIC, Institutos de Investigación de Paterna, Aptdo. 22085, 46071 Valencia, Spain; Department of Physics, Guangxi Normal University, Guilin 541004, ChinaWe perform a theoretical study of the χcJ→ϕK⁎K¯→ϕKπK¯ reaction taking into account the K⁎K¯ final state interaction, which in the chiral unitary approach is responsible, together with its coupled channels, for the formation of the low lying axial vector mesons, in this case the h1(1380) given the selection of quantum numbers. Based on this picture we can easily explain why in the χc0 decay the h1(1380) resonance is not produced, and, in the case of χc1 and χc2 decay, why a dip in the K+π0K− mass distribution appears in the 1550-1600 MeV region, that in our picture comes from a destructive interference between the tree level mechanism and the rescattering that generates the h1(1380) state. Such a dip is not reproduced in pictures where the nominal h1(1380) signal is added incoherently to a background, which provides support to the picture where the resonance appears from rescattering of vector-pseudoscalar components.http://www.sciencedirect.com/science/article/pii/S0370269319305453 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Sheng-Juan Jiang S. Sakai Wei-Hong Liang E. Oset |
spellingShingle |
Sheng-Juan Jiang S. Sakai Wei-Hong Liang E. Oset The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonances Physics Letters B |
author_facet |
Sheng-Juan Jiang S. Sakai Wei-Hong Liang E. Oset |
author_sort |
Sheng-Juan Jiang |
title |
The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonances |
title_short |
The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonances |
title_full |
The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonances |
title_fullStr |
The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonances |
title_full_unstemmed |
The χcJ decay to ϕK⁎K¯,ϕh1(1380) testing the nature of axial vector meson resonances |
title_sort |
χcj decay to ϕk⁎k¯,ϕh1(1380) testing the nature of axial vector meson resonances |
publisher |
Elsevier |
series |
Physics Letters B |
issn |
0370-2693 |
publishDate |
2019-10-01 |
description |
We perform a theoretical study of the χcJ→ϕK⁎K¯→ϕKπK¯ reaction taking into account the K⁎K¯ final state interaction, which in the chiral unitary approach is responsible, together with its coupled channels, for the formation of the low lying axial vector mesons, in this case the h1(1380) given the selection of quantum numbers. Based on this picture we can easily explain why in the χc0 decay the h1(1380) resonance is not produced, and, in the case of χc1 and χc2 decay, why a dip in the K+π0K− mass distribution appears in the 1550-1600 MeV region, that in our picture comes from a destructive interference between the tree level mechanism and the rescattering that generates the h1(1380) state. Such a dip is not reproduced in pictures where the nominal h1(1380) signal is added incoherently to a background, which provides support to the picture where the resonance appears from rescattering of vector-pseudoscalar components. |
url |
http://www.sciencedirect.com/science/article/pii/S0370269319305453 |
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