Tentative estimates of $\mathcal{B}(X(3872)\toπ^0π^0χ_{c1})$ and $\mathcal{B}(X(3872)\toπ^+π^-χ_{c1})$

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Hauptverfasser: Achasov, N. N., Shestakov, G. N.
Format: Preprint
Veröffentlicht: 2024
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author Achasov, N. N.
Shestakov, G. N.
author_facet Achasov, N. N.
Shestakov, G. N.
contents The rates of the $X(3872)\toπ^0π^0χ_{c1}$ and $X(3872)\to π^+π^-χ_{c1}$ decays are estimated in the model of the triangle loop diagrams with charmed $D^*\bar DD$ and $\bar D^*D\bar D$ mesons in the loops. There are the triangle logarithmic singularities in the physical region of the $X(3872)\toπ^0π^0 χ_{c1}$ decay which manifest themselves as narrow peaks in the $π^0χ_{c1}$ mass spectrum near the $D^0\bar D^0$ threshold. The model predicts approximately the same branching fractions of the $X(3872)\toπ^0π^0 χ_{c1}$ and $X(3872)\toπ^+π^-χ_{c1}$ decays at the level of about (0.8-1.7)$\times10^{-4}$. A distinct prediction of the model is the value of the ratio $\mathcal{R}= \mathcal{B}(X(3872)\toπ^+π^-χ_{c1})/\mathcal{B}(X(3872) \toπ^0π^0χ_{c1})\approx1.1$. It weakly depends on the $X(3872)$ resonance parameters and indicates a significant violation of the isotopic symmetry according to which one would expect $\mathcal{R}=2$.
format Preprint
id arxiv_https___arxiv_org_abs_2405_09228
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Tentative estimates of $\mathcal{B}(X(3872)\toπ^0π^0χ_{c1})$ and $\mathcal{B}(X(3872)\toπ^+π^-χ_{c1})$
Achasov, N. N.
Shestakov, G. N.
High Energy Physics - Phenomenology
High Energy Physics - Experiment
Nuclear Experiment
Nuclear Theory
The rates of the $X(3872)\toπ^0π^0χ_{c1}$ and $X(3872)\to π^+π^-χ_{c1}$ decays are estimated in the model of the triangle loop diagrams with charmed $D^*\bar DD$ and $\bar D^*D\bar D$ mesons in the loops. There are the triangle logarithmic singularities in the physical region of the $X(3872)\toπ^0π^0 χ_{c1}$ decay which manifest themselves as narrow peaks in the $π^0χ_{c1}$ mass spectrum near the $D^0\bar D^0$ threshold. The model predicts approximately the same branching fractions of the $X(3872)\toπ^0π^0 χ_{c1}$ and $X(3872)\toπ^+π^-χ_{c1}$ decays at the level of about (0.8-1.7)$\times10^{-4}$. A distinct prediction of the model is the value of the ratio $\mathcal{R}= \mathcal{B}(X(3872)\toπ^+π^-χ_{c1})/\mathcal{B}(X(3872) \toπ^0π^0χ_{c1})\approx1.1$. It weakly depends on the $X(3872)$ resonance parameters and indicates a significant violation of the isotopic symmetry according to which one would expect $\mathcal{R}=2$.
title Tentative estimates of $\mathcal{B}(X(3872)\toπ^0π^0χ_{c1})$ and $\mathcal{B}(X(3872)\toπ^+π^-χ_{c1})$
topic High Energy Physics - Phenomenology
High Energy Physics - Experiment
Nuclear Experiment
Nuclear Theory
url https://arxiv.org/abs/2405.09228