In the present work, we study the radiative decays of the P-wave $D\bar{D}^*$ molecular state $G_0$ with $I^G(J^{PC})=0^+(0^{-+})$ using a phenomenological Lagrangian approach. The molecular coupling is fixed by the compositeness condition with a Gaussian form factor. The partial widths for $G_0\to \gamma\gamma$, $\gamma J/\psi$, $\gamma \psi(2S)$, $\gamma h_c$, $\gamma \rho$, and $\gamma \omega$ are evaluated. Our results show that the two-photon and $\gamma h_c$ channels are highly suppressed, while $\gamma J/\psi$, $\gamma \psi(2S)$, and $\gamma \rho$ are of the order of a few keV, and $\gamma \omega$ reaches several tens of keV, making it the dominant radiative mode. The ratios $\Gamma(G_0 \to \gamma \psi(2S))/\Gamma(G_0 \to \gamma J/\psi)$ and $\Gamma(G_0 \to \gamma \omega)/\Gamma(G_0 \to \gamma \rho)$ are predicted to be 1-2.6 and 3.4-5.4, respectively, with mild parameter dependence. We also compare with hadronic decays and find that the total radiative decay width is lower than the hadronic decay widths by about one order of magnitude. We propose searching for $G_0$ in the sequential decay $Y(4230)\to \gamma G_0 \to \gamma\omega J/\psi$, which is accessible to further experimental measurements by the BESIII, Belle II and LHCb Collaborations.
We study radiative double-charmonium production, $e^+e^-\to HH\gamma$ with $H=J/\psi$ and $\eta_c$, at $\sqrt{s}=10.58~{\rm GeV}$, including a possible tensor contribution from the fully charmed state $X(6900)$. The nonresonant amplitudes are calculated within the color-singlet non-relativistic QCD framework, while the...
Meng Jia, Yi-Jie Li, Guang-Hua Xu et al.· 1 citation
Using $2712.4 \pm 14.3$ million $\psi(3686)$ events collected with the BESIII detector, the $\Lambda\bar{\Lambda}$ system produced in $\psi(3686)$ radiative decays is studied. A model-independent partial wave analysis reveals a significant threshold enhancement structure dominated by the $^1S_0$ and $^3P_0$ partial wav...
Besiii Collaboration M. Ablikim, M. N. Achasov, P. Adlarson et al.· 0 citations
Inspired by the recent observation of the $\Sigma_c(3200)^0$ baryon in the $\Lambda_c^+\pi^-$ invariant mass spectrum by the LHCb Collaboration, we perform a comprehensive investigation of the $D^{(*)}\Delta$ interactions within the one-boson-exchange framework. Our results show that the $D^*\Delta$ molecule with $I(J^...
We investigate the relative $P$-wave excitations of the $D^{(*)}\bar D^{(*)}$ systems using the QCD sum rule method. By introducing a covariant derivative between two ground-state charmed meson fields, we construct color-singlet interpolating currents to describe the relative orbital excitation between the two meson cl...
Yi-Wei Jiang, Hua-Xing Chen, Er-Liang Cui et al.· 0 citations
In the hadronic molecular picture, an isoscalar $S$-wave $D\bar{D}$ molecule is naturally expected as the spin-0 partner of $X(3872)$. Assuming this state, denoted by $X_0$, to be a pure $D\bar D$ molecule with quantum numbers $J^{PC}=0^{++}$, we investigate its radiative decays $X_0\to\gamma V (V=\rho^0,\omega)$ withi...
Yuan Gao, Gang Li, Shi-Dong Liu et al.· 0 citations
We report on two recent calculations on the inclusive radiative decay $\bar B\to X_s \gamma$, notably multi-parton contributions at NLO and the $Q_{1,2}-Q_7$ interference at NNLO for the physical value of the charm-quark mass. The former calculation formally completes $\bar{B} \rightarrow X_s \gamma$ at NLO in QCD at l...
T. Huber· Proceedings of Loops and Leg...· 0 citations
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