3,569 research outputs found

    Search for the Lepton Flavor Violation Process J/ψeμJ/\psi \to e\mu at BESIII

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    We search for the lepton-flavor-violating decay of the J/ψJ/\psi into an electron and a muon using (225.3±2.8)×106(225.3\pm2.8)\times 10^{6} J/ψJ/\psi events collected with the BESIII detector at the BEPCII collider. Four candidate events are found in the signal region, consistent with background expectations. An upper limit on the branching fraction of B(J/ψeμ)<1.5×107\mathcal{B}(J/\psi \to e\mu)< 1.5 \times 10^{-7} (90% C.L.) is obtained

    Measurement of the e+eπ+π\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation

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    We extract the e+eπ+πe^+e^-\rightarrow \pi^+\pi^- cross section in the energy range between 600 and 900 MeV, exploiting the method of initial state radiation. A data set with an integrated luminosity of 2.93 fb1^{-1} taken at a center-of-mass energy of 3.773 GeV with the BESIII detector at the BEPCII collider is used. The cross section is measured with a systematic uncertainty of 0.9%. We extract the pion form factor Fπ2|F_\pi|^2 as well as the contribution of the measured cross section to the leading order hadronic vacuum polarization contribution to (g2)μ(g-2)_\mu. We find this value to be aμππ,LO(600900  MeV)=(368.2±2.5stat±3.3sys)1010a_\mu^{\pi\pi,\rm LO}(600-900\;\rm MeV) = (368.2 \pm 2.5_{\rm stat} \pm 3.3_{\rm sys})\cdot 10^{-10}.Comment: 14 pages, 7 figures, accepted by PL

    Observation of J/ψppˉa0(980)J/\psi \rightarrow p\bar{p}a_{0}(980) at BESIII

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    Using 2.25×1082.25\times10^{8} J/ψJ/\psi events collected with the BESIII detector at the BEPCII storage rings, we observe for the first time the process J/ψppˉa0(980)J/\psi\rightarrow p\bar{p}a_{0}(980), a0(980)π0ηa_{0}(980)\rightarrow \pi^{0}\eta with a significance of 6.5σ6.5\sigma (3.2σ3.2\sigma including systematic uncertainties). The product branching fraction of J/ψppˉa0(980)ppˉπ0ηJ/\psi\rightarrow p\bar{p}a_{0}(980)\rightarrow p\bar{p}\pi^{0}\eta is measured to be (6.8±1.2±1.3)×105(6.8\pm1.2\pm1.3)\times 10^{-5}, where the first error is statistical and the second is systematic. This measurement provides information on the a0a_{0} production near threshold coupling to ppˉp\bar{p} and improves the understanding of the dynamics of J/ψJ/\psi decays to four body processes.Comment: 8 pages, 7 figure

    Precision measurement of the D0D^{*0} decay branching fractions

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    Using 482 pb1^{-1} of data taken at s=4.009\sqrt{s}=4.009 GeV, we measure the branching fractions of the decays of D0D^{*0} into D0π0D^0\pi^0 and D0γD^0\gamma to be \BR(D^{*0} \to D^0\pi^0)=(65.5\pm 0.8\pm 0.5)% and \BR(D^{*0} \to D^0\gamma)=(34.5\pm 0.8\pm 0.5)% respectively, by assuming that the D0D^{*0} decays only into these two modes. The ratio of the two branching fractions is \BR(D^{*0} \to D^0\pi^0)/\BR(D^{*0} \to D^0\gamma) =1.90\pm 0.07\pm 0.05, which is independent of the assumption made above. The first uncertainties are statistical and the second ones systematic. The precision is improved by a factor of three compared to the present world average values

    Measurement of B(ψ(3770)γχc1)\mathcal B(\psi(3770)\to\gamma \chi_{c1}) and search for ψ(3770)γχc2\psi(3770)\to\gamma \chi_{c2}

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    We report a measurement of the branching fraction of ψ(3770)γχc1\psi(3770)\to\gamma\chi_{c1} and search for the transition ψ(3770)γχc2\psi(3770)\rightarrow \gamma \chi_{c2} based on 2.92~fb1^{-1} of e+ee^+e^- data accumulated at s=3.773\sqrt{s}=3.773~GeV with the BESIII detector at the BEPCII collider. The measured branching fraction of ψ(3770)γχc1\psi(3770) \rightarrow \gamma \chi_{c1} is B(ψ(3770)γχc1)=(2.48±0.15±0.23)×103\mathcal B(\psi(3770) \rightarrow \gamma \chi_{c1})=(2.48 \pm 0.15 \pm 0.23) \times 10^{-3}, which is the most precise measurement to date. The upper limit on the branching fraction of ψ(3770)γχc2\psi(3770)\rightarrow \gamma \chi_{c2} at a 90%90\% confidence level is B(ψ(3770)γχc2)<0.64×103\mathcal B(\psi(3770) \rightarrow \gamma \chi_{c2})<0.64 \times 10^{-3}. The corresponding partial widths are Γ(ψ(3770)γχc1)=(67.5±4.1±6.7)\Gamma(\psi(3770) \to \gamma \chi_{c1}) =(67.5\pm 4.1\pm 6.7)~keV and Γ(ψ(3770)γχc2)<17.4\Gamma(\psi(3770) \to \gamma \chi_{c2}) < 17.4~keV

    Evidence for e+eγχc1,2e^+e^-\to\gamma\chi_{c1, 2} at center-of-mass energies from 4.009 to 4.360 GeV

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    Using data samples collected at center-of-mass energies of s\sqrt{s} = 4.009, 4.230, 4.260, and 4.360 GeV with the BESIII detector operating at the BEPCII collider, we perform a search for the process e+eγχcJe^+e^-\to\gamma\chi_{cJ} (J=0,1,2)(J = 0, 1, 2) and find evidence for e+eγχc1e^+e^-\to\gamma\chi_{c1} and e+eγχc2e^+e^-\to\gamma\chi_{c2} with statistical significances of 3.0σ\sigma and 3.4σ\sigma, respectively. The Born cross sections σB(e+eγχcJ)\sigma^{B}(e^+e^-\to\gamma\chi_{cJ}), as well as their upper limits at the 90% confidence level are determined at each center-of-mass energy.Comment: 8 pages, 7 figures, 3 table

    Observation of ηωe+e\eta^{\prime}\to\omega e^{+} e^{-}

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    Based on a sample of \etapr mesons produced in the radiative decay J/ψγηJ/\psi\to\gamma\eta^{\prime} in 1.31×1091.31\times 10^9 J/ψJ/\psi events collected with the BESIII detector, the decay ηωe+e\eta^{\prime}\to\omega e^{+} e^{-} is observed for the first time, with a statistical significance of 8σ8\sigma. The branching fraction is measured to be B(ηωe+e)=(1.97±0.34(stat)±0.17(syst))×104\mathcal{B}(\eta^{\prime}\to\omega e^{+} e^{-})=(1.97\pm0.34(\text{stat})\pm0.17(\text{syst}))\times10^{-4}, which is in agreement with theoretical predictions. The branching fraction of ηωγ\eta^{\prime}\to\omega\gamma is also measured to be (2.55±0.03(stat)±0.16(syst))×102(2.55\pm0.03(\text{stat})\pm0.16(\text{syst}))\times10^{-2}, which is the most precise measurement to date, and the relative branching fraction B(ηωe+e)B(ηωγ)\frac{\mathcal{B}(\eta^{\prime}\to \omega e^{+}e^{-})}{\mathcal{B}(\eta^{\prime}\to \omega \gamma)} is determined to be (7.71±1.34(stat)±0.54(syst))×103(7.71\pm1.34(\text{stat})\pm0.54(\text{syst}))\times10^{-3}.Comment: 8 pages, 10 figure

    Search for the isospin violating decay Y(4260)J/ψηπ0Y(4260)\rightarrow J/\psi \eta \pi^{0}

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    Using data samples collected at center of mass energies of s\sqrt{s} = 4.009, 4.226, 4.257, 4.358, 4.416 and 4.599 GeV with the BESIII detector operating at the BEPCII storage ring, we search for the isospin violating decay Y(4260)J/ψηπ0Y(4260)\rightarrow J/\psi \eta \pi^{0}. No signal is observed, and upper limits on the cross section σ(e+eJ/ψηπ0)\sigma(e^{+}e^{-}\rightarrow J/\psi \eta \pi^{0}) at the 90\% confidence level are determined to be 3.6, 1.7, 2.4, 1.4, 0.9 and 1.9 pb, respectively.Comment: 7 pages, 2 figure
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