Resonant structures in the dipion mass spectrum from $\chi_{c1}(3872)\to\pi^+\pi^- J/\psi$ decays, produced via $B^+\to K^+\chi_{c1}(3872)$ decays, are analyzed using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9 $fb^{-1}$. A sizeable contribution from the isospin conserving $\chi_{c1}(3872)\to\omega J/\psi$ decay is established for the first time, $(21.4\pm2.3\pm2.0)\%$, with a significance of more than $7.1\sigma$. The amplitude of isospin violating decay, $\chi_{c1}(3872)\to\rho^0 J/\psi$, relative to isospin conserving decay, $\chi_{c1}(3872)\to\omega J/\psi$, is properly determined, and it is a factor of six larger than expected for a pure charmonium state.
Distribution of $m_{\pi ^+ \pi ^- { J \mskip -3mu/\mskip -2mu\psi } }$ ($m_{ K ^+ \pi ^+ \pi ^- { J \mskip -3mu/\mskip -2mu\psi } }$ in the inset) from $ B ^+ \rightarrow K ^+ \pi ^+ \pi ^- { J \mskip -3mu/\mskip -2mu\psi } $ candidates within $\pm2 \sigma$ around the $ B ^+ $ ($\chi _{c1}(3872) $) mass, overlaid with the fit including the total (solid blue), signal (dashed red) and background (dashed green) components. |
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Distribution of $m_{\pi ^+ \pi ^- }$ in $\chi _{c1}(3872) \rightarrow \pi ^+ \pi ^- { J \mskip -3mu/\mskip -2mu\psi } $ decays, fit with the $\rho ^0 $-only model. |
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Distribution of $m_{\pi ^+ \pi ^- }$ in $\chi _{c1}(3872) \rightarrow \pi ^+ \pi ^- { J \mskip -3mu/\mskip -2mu\psi } $ decays, fit with the default $K$-matrix model. |
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Distribution of $m_{\pi ^+ \pi ^- }$ in $\chi _{c1}(3872) \rightarrow \pi ^+ \pi ^- { J \mskip -3mu/\mskip -2mu\psi } $ decays, fit with the Gounaris--Sakurai model. The dashed line represents the $\rho'$ contribution multiplied by a factor of 10. |
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Amplitude model for $\chi _{c1}(3872) \rightarrow \pi ^+ \pi ^- { J \mskip -3mu/\mskip -2mu\psi } $ decays, obtained by the default fit to the LHCb data (Fig. 3), with the phase-space integration limit extended by setting the $\chi _{c1}(3872) $ mass to $4000 \text{ Me V} $. The actual phase-space limit, imposed by the measured $\chi _{c1}(3872) $ mass, is indicated by the vertical dashed line. Neither mass resolution nor detector efficiency are applied here. |
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Animated gif made out of all figures. |
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Results for $\omega$ fractions with systematic uncertainties. See text for a description of the individual entries. |
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Created on 26 April 2024.