SearcharxivSearch

arXiv subjects

Xiao-Yu Qi

Publications and source records attributed to Xiao-Yu Qi.

3 recordsLinked to original sources

The light meson decays of $D$ wave charmonia

Motivated by the large non-$D\bar{D}$ branching fraction of $ψ(3770)$, we investigate the light meson decays of the $D$-wave charmonia in the present work with the meson loop mechanism. With the parameter range determined by $ψ(3770) \to ϕη$, our estimations of the branching fractions of the light meson decays of $ψ(3770)$ are consistent with the estimations in the literature. As for $ψ(3823)$, the partial widths of $K^\ast \bar{K}^\ast$ channel is estimated to be around 200 keV, which is the the predominant light meson decay channel of $ψ(3823)$. Our estimations also indicate that $K^{(\ast)}\bar{K}^{(\ast)}$ and $ρπ$ are the dominant light meson decay modes of $ψ(3842)$, while $η_{c2}$ dominantly decays into $ρρ$, $K^\ast \bar{K}^\ast$, $ωω$ and $ϕϕ$.

hep-ph

Two-body Hidden Charm Decays of $D$ Wave Charmonia

The experimental observations of $ψ_2(3823)$ and $ψ_3(3842)$ make $D$ wave charmonia family abundant. In the present work, we investigate the hidden charm decay processes of spin triplets of the $D$-wave charmonia with the meson loop mechanism. The model parameter $α_Λ$ is determined by reproducing the branching fraction of $ψ(3770)\to J/ψη$. With this range of model parameter values, the branching fractions (partial widths) of $ψ(3770) \to η_c ω$, $ψ_2(3823)/ψ_3(3842) \to J/ψη$, $ψ_2(3823)/ψ_3(3842) \to η_c ω$ are estimated. Our estimations find that the partial width of $ψ_2(3823) \to J/ψη$ is $\left(29.64^{+4.01}_{-4.63}\right)\ \mathrm{keV}$, and the partial width ratio of $ψ_2(3823) \to J/ψη$ relative to $ψ_2(3823)\to γχ_{c1}$ is about $10\%$, which could be tested by further precise measurements from the BESIII, Belle II and LHCb Collaborations.

hep-ph

Pionic transitions from $Z_c(4020)$ to $D$ wave charmonia

In the present work, we investigate the charmed meson loops contributions to the pionic transitions from $Z_c(4020)^+$ to the $D$ wave triplets charmonia by using an effective Lagrangian approach. Our estimations indicate that the predicted branching fraction of $Z_c(4020)^+ \to π^+ ψ(1^3D_J) , \ J=(1,2,3)$ are much smaller than the one of $Z_c(4020)^+ \to π^+ h_c $. Thus, searching $Z_c(4020)^\pm$ in the $π^\pm ψ(1^3D_J) $ invariant mass distributions is impossible. Thus, the observed peak structures at 4.04 and 4.13 GeV in the $π^\pm ψ(3770)$ invariant mass distributions should not come from the contributions of $Z_c(4020)^\pm$, and further precise experimental measurements of the $e^+ e^- \to π^+ π^- ψ(3770)$ process are needed to decode the nature of these two peak structures.

hep-ph