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The processes $X(3872)to D^{*0}bar{D^{0}}+c.c.,~gamma J/psi,~gamma psi(2S),$ and $gamma D^{+}D^{-}$ are searched for in a $9.0~rm fb^{-1}$ data sample collected at center-of-mass energies between $4.178$ and $4.278$ GeV with the BESIII detector. We observe $X(3872)to D^{*0}bar{D^{0}}+c.c.$ and find evidence for $X(3872)togamma J/psi$ with statistical significances of $7.4sigma$ and $3.5sigma$, respectively. No evident signals for $X(3872)togammapsi(2S)$ and $gamma D^{+}D^{-}$ are found, and upper limit on the relative branching ratio $R_{gamma psi} equivfrac{mathcal{B}(X(3872)togammapsi(2S))}{mathcal{B}(X(3872)togamma J/psi)}<0.59$ is set at 90$%$ confidence level. Measurements of branching ratios relative to decay $X(3872)topi^+pi^- J/psi$ are also reported for decays $X(3872)to D^{*0}bar{D^{0}}+c.c., ~gammapsi(2S),~gamma J/psi$, $gamma D^{+}D^{-}$, as well as the non-$D^{*0}bar{D}^{0}$ three-body decays $pi^0 D^{0}bar{D}^{0}$ and $gamma D^{0}bar{D}^{0}$.
We present results on the X(3872), produced in $B^+ to X(3872) K^+$ and $B^0 to X(3872) K^0_S$ decays where $X(3872) to J/psi pi^+ pi^-$. We report the first statistically significant observation of $B^0 to X(3872) K^0_S$ and measure the ratio of bra
We discuss the possibilities of producing the X(3872), which is assumed to be a D bar D^* bound state, in radiative decays of charmonia. We argue that the ideal energy regions to observe the X(3872) associated with a photon in e^+e^- annihilations ar
We report the first observation of $B^0 to X(3872) (K^{+}pi^{-})$ and evidence for $B^+ to X(3872) (K^{0}pi^{+})$. We measure the product of branching fractions for the former to be ${cal B}(B^0 to X(3872) (K^+ pi^-)) times {cal B}(X(3872) to J/psi p
We report a study of $Bto (J/psi gamma) K$ and $Bto (psi gamma)K$ decay modes using $772times 10^{6}$ $Bbar{B}$ events collected at the Upsilon(4S)$ resonance with the Belle detector at the KEKB energy-asymmetric $e^+ e^-$ collider. We observe $X(387
We present measurements of the decays B+ -> X(3872) K+ and B0 -> X(3872) K0 with X(3872) -> Jpsi pi+ pi-. The data sample used, collected with the BABAR detector at the PEP-II e+e- asymmetric-energy storage ring, corresponds to 455 x 10^6 BBbar pairs