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Evidence of the open-flavor tetraquark T_{cbar{s}2} in the process B^+to D^(*-)D_s^+π^+
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Evidence of the open-flavor tetraquark T_{cbar{s}2} in the process B^+to D^(*-)D_s^+π^+
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The newly observed open-flavor tetraquark $T_{c\bar{s}0}(2900)$ has attracted many attentions, and searching for its spin partners is crucial to exploring the internal structure of those states. In this work, we will show that, the $D_s^+\pi^+$ invariant mass distribution of the process $B^+\to D^{*-}D_s^+\pi^+$ measured by LHCb has a resonant-like structure around 2830~MeV, which could be associated with the predicted $T_{c\bar{s}2}$, the spin $J=2$ partner of $T_{c\bar{s}0}(2900)$. Furthermore, we have evaluated the momenta of the angular mass distribution, which are very different for each of the spin assumptions, and have larger strength at the resonant energy than the peaks seen in the angular integrated mass distribution. We make a call for the experimental determination of these magnitudes, which could be used to pin down the existence of the $T_{c\bar{s}2}$.
Forward citations
Cited by 2 Pith papers
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Exotic $T^*_{csJ}$ and $T^*_{c\bar{s}J}$ states and coupled-channel scattering at the $SU(3)$ flavour symmetric point from lattice QCD
First lattice QCD calculation at the SU(3) flavour symmetric point finds poles in exotic charm-light meson scattering amplitudes, linking a J^P=0+ resonance to experimental T*cs0(2870)^0 and T*c s-bar0(2900) states an...
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Discovering the Gell-Mann-Okubo Formula with Kolmogorov-Arnold Networks
A KAN network's fitted polynomials are hand-rearranged into the known Gell-Mann-Okubo mass relations, so the claimed autonomous rediscovery is not demonstrated.
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