X(3872) revisited: the roles of OPEP and the quark degrees of freedom

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Main Authors: Takeuchi, Sachiko, Yamaguchi, Yasuhiro, Hosaka, Atsushi, Takizawa, Makoto
Format: Preprint
Published: 2024
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_version_ 1866914813133717504
author Takeuchi, Sachiko
Yamaguchi, Yasuhiro
Hosaka, Atsushi
Takizawa, Makoto
author_facet Takeuchi, Sachiko
Yamaguchi, Yasuhiro
Hosaka, Atsushi
Takizawa, Makoto
contents The $X(3872)$ is investigated by employing the quark-hadron hybrid model, that consists of the $c\bar c$ core, $D^{(*)}\bar D{}^*$, $J/ψω$, and $J/ψρ$ two-meson states. Due to the attraction from the $c\bar c$-$D\bar D{}^*$ coupling and from the OPEP tensor coupling, a very thin peak can appear at the $D^{0}\bar D{}^{*0}$ threshold. The energy of the corresponding pole of the scattering matrix is $E=(+0.06-0.14i)$ MeV, which is on the physical sheet and above the threshold, the same as the one of the poles from the LHCb data analysis.
format Preprint
id arxiv_https___arxiv_org_abs_2405_16794
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle X(3872) revisited: the roles of OPEP and the quark degrees of freedom
Takeuchi, Sachiko
Yamaguchi, Yasuhiro
Hosaka, Atsushi
Takizawa, Makoto
High Energy Physics - Phenomenology
The $X(3872)$ is investigated by employing the quark-hadron hybrid model, that consists of the $c\bar c$ core, $D^{(*)}\bar D{}^*$, $J/ψω$, and $J/ψρ$ two-meson states. Due to the attraction from the $c\bar c$-$D\bar D{}^*$ coupling and from the OPEP tensor coupling, a very thin peak can appear at the $D^{0}\bar D{}^{*0}$ threshold. The energy of the corresponding pole of the scattering matrix is $E=(+0.06-0.14i)$ MeV, which is on the physical sheet and above the threshold, the same as the one of the poles from the LHCb data analysis.
title X(3872) revisited: the roles of OPEP and the quark degrees of freedom
topic High Energy Physics - Phenomenology
url https://arxiv.org/abs/2405.16794