2ABLIKIM 2021AP fit to the cross section between 2.00 and 3.08 GeV with a sum of Breit-Wigner amplitude and a nonresonant contribution.
3LEES 2020 fit to the BABAR data of LEES 2013Q and BESIII data of ABLIKIM 2019L assuming a coherent sum of a single Breit-Wigner resonance and a non-resonant contribution.
4CHEN 2025D combined analysis of the cross sections for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}}$ and ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ using data from ABLIKIM 2019L and ABLIKIM 2021AP. The parametrisation includes CHEN 2025D the interference between direct coupling process and resonance intermediate process with the isospin factor fixed to one. Other solutions which include additional vector resonances give $85.9$ $\pm8.6$ MeV and $86.4$ $\pm8.9$ MeV.
5LEES 2020 fit to the BABAR data of LEES 2013Q assuming a coherent sum of a single Breit-Wigner resonance and a non-resonant contribution. The resonance significance is 3.5 ${{\mathit \sigma}}$.
References:
AFZAL
2026
PRL 136 251902
Search for the $Y(2175)$ in the photoproduction cross section measurement of $?p \to ??^{+} ?^{-} p$ at GlueX
CHEN
2025D
EPJ C85 1388
A combined analysis of $Y(2240)$ in the $e^+ e^- \to K^+ K^-$ and $e^+ e^- \to K_S^0 K_L^0$ processes
ABLIKIM
2021AP
PR D104 092014
Cross section measurement of $e^{+}e^{-} \to K_{S}^{0}K_{L}^{0}$ at $\sqrt{s}=2.00-3.08~{GeV}$
LEES
2020
PR D101 012011
Resonances in $e^+e^-$ annihilation near 2.2 GeV
ABLIKIM
2019L
PR D99 032001
Measurement of $e^{+} e^{-} \rightarrow K^{+} K^{-}$ cross section at $\sqrt{s} = 2.00 - 3.08$ GeV