Strong decays of the $Y(4660)$ as a vector tetraquark state in solid quark-hadron duality (1901.02177v2)
Abstract: In this article, we choose the $[sc]P[\bar{s}\bar{c}]_A-[sc]_A[\bar{s}\bar{c}]_P$ type tetraquark current to study the hadronic coupling constants in the strong decays $Y(4660)\to J/\psi f_0(980)$, $\eta_c \phi(1020)$, $\chi{c0}\phi(1020)$, $D_s\bar{D}s$, $ D_s* \bar{D}*_s$, $ D_s \bar{D}*_s$, $D_s* \bar{D}_s$, $\psi\prime \pi+\pi-$, $J/\psi\phi(1020)$ with the QCD sum rules based on solid quark-hadron quality. The predicted width $\Gamma(Y(4660) )= 74.2{+29.2}{-19.2}\,{\rm{MeV}}$ is in excellent agreement with the experimental data $68\pm 11\pm 1 {\mbox{ MeV}}$ from the Belle collaboration, which supports assigning the $Y(4660)$ to be the $[sc]P[\bar{s}\bar{c}]_A-[sc]_A[\bar{s}\bar{c}]_P$ type tetraquark state with $J{PC}=1{--}$. In calculations, we observe that the hadronic coupling constants $ |G{Y\psi\prime f_0}|\gg |G_{Y J/\psi f_0}|$, which is consistent with the observation of the $Y(4660)$ in the $\psi\prime\pi+\pi-$ mass spectrum, and favors the $\psi{\prime}f_0(980)$ molecule assignment. It is important to search for the process $Y(4660)\to J/\psi \phi(1020)$ to diagnose the nature of the $Y(4660)$, as the decay is greatly suppressed.
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