Study of \(D_{s1}(2460)^{+}\to D_{s}^{+}\pi^{+}\pi^{-}\) in \(B\to {\bar{D}}^{()}D_{s}^{+}\pi^{+}\pi^{-}\) decays
An amplitude analysis of the \(D_{s1}(2460)^+\to D_{s}^{+}\pi^{+}\pi^{-}\) transition is performed simultaneously in \(B^{0}\to D^{-}D_{s}^{+}\pi^{+}\pi^{-}\), \(B^{+}\to{\bar{D}}^{0} D_{s}^{+}\pi^{+}\pi^{-}\), and \(B^{0}\to D^{*-}D_{s}^{+}\pi^{+}\pi^{-}\) decays. The study is based on a data sampl...
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Published in | arXiv.org |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format | Paper |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
05.11.2024
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Subjects | |
Online Access | Get full text |
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Summary: | An amplitude analysis of the \(D_{s1}(2460)^+\to D_{s}^{+}\pi^{+}\pi^{-}\) transition is performed simultaneously in \(B^{0}\to D^{-}D_{s}^{+}\pi^{+}\pi^{-}\), \(B^{+}\to{\bar{D}}^{0} D_{s}^{+}\pi^{+}\pi^{-}\), and \(B^{0}\to D^{*-}D_{s}^{+}\pi^{+}\pi^{-}\) decays. The study is based on a data sample of proton-proton collisions recorded with the LHCb detector at centre-of-mass energies of \(\sqrt{s}=7,8,\) and \(13\,\)TeV, corresponding to a total integrated luminosity of \(9\,\rm{fb}^{-1}\). A clear double-peak structure is observed in the \(m(\pi^{+}\pi^{-})\) spectrum of the \(D_{s1}(2460)^{+}\to D_{s}^{+}\pi^{+}\pi^{-}\) decay. The data can be described either with a model including \(f_0(500)\), \(f_0(980)\) and \(f_2(1270)\) resonances, in which the contributions of \(f_0(980)\) and \(f_2(1270)\) are unexpectedly large, or with a model including \(f_0(500)\), a doubly charged open-charm tetraquark state \(T_{c\bar{s}}^{++}\) and its isospin partner \(T_{c\bar{s}}^{0}\). If the former is considered implausible, the \(T_{c\bar{s}}\) states are observed with high significance, and the data are consistent with isospin symmetry. When imposing isospin constraints between the two \(T_{c\bar{s}}\) states, their mass and width are determined to be \(2327\pm13\pm13\,\)MeV and \(96\pm16\,^{+170}_{-23}\,\)MeV, respectively, where the first uncertainty is statistical and the second is systematic. The mass is slightly below the \(DK\) threshold, and a spin-parity of \(0^+\) is favoured with high significance. |
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ISSN: | 2331-8422 |