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Evidence of a $J/\psi K_{\rm S}^0$ structure in $B^0 \to J/\psi \phi K_{\rm S}^0$ decays

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Abstract

An amplitude analysis of $B^0 \to J/\psi \phi K_S^0$ decays is performed using proton-proton collision data corresponding to an integrated luminosity of 9 ${\rm fb}^{-1}$, collected with the LHCb detector at centre-of-mass energies of 7, 8 and 13 TeV. Evidence with a significance of $4.0$ standard deviations of a structure in the $J/\psi K_S^0$ system, named $T_{\psi s1}^{\theta}(4000)^0$, is seen, with its mass and width measured to be $3991 _{-10}^{+12} ^{+\phantom{0}9}_{-17}$ MeV and $105 _{-25}^{+29} ^{+17}_{-23}$ MeV, respectively, where the first uncertainty is statistical and the second systematic. The $T_{\psi s1}^{\theta}(4000)^0$ state is likely to be the isospin partner of the $T_{\psi s1}^{\theta}(4000)^+$ state, previously observed in the $J/\psi K^+$ system of the $B^+ \to J/\psi \phi K^+$ decay. When isospin symmetry for the charged and neutral $T_{\psi s1}^{\theta}(4000)$ states, is assumed, the signal significance increases to $5.4$ standard deviations.

Figures and captions

(a) Invariant-mass distribution of selected $ B ^0$ candidates and corresponding fit result. (b) Distribution of $m^2_{ { J \mskip -3mu/\mskip -2mu\psi } K ^0_{\mathrm{S}} }$ versus $m^2_{ { J \mskip -3mu/\mskip -2mu\psi } \phi}$ for candidates in the $\pm$15 $\text{ Me V}$ region around the nominal $ B ^0 $ mass.

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Distributions of (left) $m_{\phi K}$, (middle) $m_{ { J \mskip -3mu/\mskip -2mu\psi } \phi}$, and (right) $m_{ { J \mskip -3mu/\mskip -2mu\psi } K}$, overlaid with the corresponding projections of the default fit model. The upper and lower rows correspond to the $ B ^+ \rightarrow { J \mskip -3mu/\mskip -2mu\psi } \phi K ^+ $ and $ B ^0 \rightarrow { J \mskip -3mu/\mskip -2mu\psi } \phi K ^0_{\mathrm{S}} $ decays, respectively.

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Tables and captions

Results for the $ T_{\psi s1}^{\theta}(4000)^0$ state from the default model. The first uncertainty is statistical and the second systematic.

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Systematic uncertainties associated to the mass, width, fit fraction of the $ T_{\psi s1}^{\theta}(4000)^0$ state, and the mass difference between the $ T_{\psi s1}^{\theta}(4000)^0$ and $ T_{\psi s1}^{\theta}(4000)^+$ states.

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Supplementary Material [file]

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Created on 19 April 2024.