Search results for "Γee"

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An improved limit for Γee of X(3872) and Γee measurement of ψ(3686)

2015

Using the data sets taken at center-of-mass energies above 4 GeV by the BESIII detector at the BEPCII storage ring, we search for the reaction e+e−→γISRX(3872)→γISRπ+π−J/ψ via the Initial State Radiation technique. The production of a resonance with quantum numbers JPC=1++ such as the X(3872) via single photon e+e− annihilation is forbidden, but is allowed by a next-to-leading order box diagram. We do not observe a significant signal of X(3872) , and therefore give an upper limit for the electronic width times the branching fraction ΓeeX(3872)B(X(3872)→π+π−J/ψ)<0.13 eV at the 90% confidence level. This measurement improves upon existing limits by a factor of 46. U…

Nuclear and High Energy PhysicsX(3872)BESIII; Charmonium spectroscopy; X(3872); Γ; ee; ψ(3686)ψ(3686)ΓBESIIIBESIII; Charmonium spectroscopy; X(3872); Γee; ψ(3686); Nuclear and High Energy PhysicsCharmonium spectroscopyΓeeeelcsh:Physicslcsh:QC1-999
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An improved limit for Γee of X(3872) and Γee measurement of ψ(3686)

2015

Çetin, Serkant Ali (Dogus Author) Using the data sets taken at center-of-mass energies above 4 GeV by the BESIII detector at the BEPCII storage ring, we search for the reaction e+e-→γISRX(3872)→γISRπ+π-J/ψ via the Initial State Radiation technique. The production of a resonance with quantum numbers JPC=1++ such as the X(3872) via single photon e+e- annihilation is forbidden, but is allowed by a next-to-leading order box diagram. We do not observe a significant signal of X(3872), and therefore give an upper limit for the electronic width times the branching fraction ΓeeX(3872)B(X(3872)→π+π-J/ψ)<0.13 eV at the 90% confidence level. This measurement improves upon existing limits by a factor of…

X(3872)ψ(3686)BESIIIΓeeCharmonium Spectroscopy
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