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Shedding light on the X(3930) X(3930) and X(3960) X(3960) states with the BKJ/ψωB^- \to K^- J/ψω reaction

Published 17 Feb 2023 in hep-ph | (2302.08877v2)

Abstract: We have studied the contribution of the state X(3930)X(3930), coming from the interaction of the DDD \overline{D} and D<sup>+s</sup>D<sup>sD<sup>{+}_s</sup> D<sup>{-}_s channels, to the B<sup></sup>K<sup></sup>J/ψωB<sup>-</sup> \to K<sup>-</sup> J/\psi \omega decay. The purpose of this work is to offer a complementary tool to see if the X(3930)X(3930) state observed in the D<sup>+</sup>D<sup>D<sup>+</sup> D<sup>- channel is the same or not as the X(3960)X(3960) resonance claimed by the LHCb collaboration from a peak in the D<sup>+s</sup>D<sup>sD<sup>{+}_s</sup> D<sup>{-}_s mass distribution around threshold. We present results for what we expect in the J/ψωJ/\psi \omega mass distribution in the B<sup></sup>K<sup></sup>J/ψωB<sup>-</sup> \to K<sup>-</sup> J/\psi \omega decay and conclude that a clear signal should be seen around 3930MeV3930\,\rm MeV. At the same time, finding no extra resonance signal at 3960MeV3960\,\rm MeV would be a clear indication that there is not a new state at 3960MeV3960\,\rm MeV, supporting the hypothesis that the near-threshold peaking structure peak in the D<sup>+s</sup>D<sup>sD<sup>{+}_s</sup> D<sup>{-}_s mass distribution is only a manifestation of a resonance below threshold.

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