16 research outputs found

    Observation of Electromagnetic Dalitz decays J/ψ\to P e^+e^-

    Get PDF
    Based on a sample of (225.3\pm2.8)\times 10^{6} J/\psi events collected with the BESIII detector, the electromagnetic Dalitz decays of J/\psi \to P e^+e^-(P=\eta'/\eta/\pi^0) are studied. By reconstructing the pseudoscalar mesons in various decay modes, the decays J/\psi \to \eta' e^+e^-, J/\psi \to \eta e^+e^- and J/\psi \to \pi^0 e^+e^- are observed for the first time. The branching fractions are determined to be \mathcal{B}(J/\psi\to \eta' e^+e^-) = (5.81\pm0.16\pm0.31)\times10^{-5}, \mathcal{B}(J/\psi\to \eta e^+e^-) = (1.16\pm0.07\pm0.06)\times10^{-5}, and \mathcal{B}(J/\psi\to \pi^0 e^+e^-)=(7.56\pm1.32\pm0.50)\times10^{-7}, where the first errors are statistical and the second ones systematic

    "Table 2" of "Evidence for e+e−→γχc1,2e^+e^-\to\gamma\chi_{c1, 2} at center-of-mass energies from 4.009 to 4.360 GeV"

    No full text
    The results on e+e−→γχc1e^+e^-\to\gamma\chi_{c1} Born cross section measurement. Shown in the table are the significance σ\sigma, detection efficiency ϵ\epsilon, number of signal events from the fits Nobs^{\rm obs}, radiative correction factor (1+δr1+\delta^{r}), vacuum polarization factor (1+δv1+\delta^{v}), upper limit (at the 90%\% C.L.) on the number of signal events NUP^{\rm UP}, Born cross section σB\sigma^{B} and upper limit (at the 90%\% C.L.) on the Born cross section σUP\sigma^{\rm UP} at different CME points

    "Table 1" of "Study of e+e−→ppˉe^+e^- \rightarrow p\bar{p} in the vicinity of ψ(3770)\psi(3770)"

    No full text
    Summary of results at center-of-mass energies from 3.65 to 3.90 GeV. N(SIG) is the number of E+ E- --> P P events; EPSILON is the detection efficiency; L is the integrated luminosity; (1 + DELTA)(DRESSED) is the initial state radiation correction factor without the vacuum polarization correction; and SIG(OBS), SIG(DRESSED) and SIG(BORN) are the observed cross section, the dressed cross section and the Born cross section, respectively

    "Table 3" of "Evidence for e+e−→γχc1,2e^+e^-\to\gamma\chi_{c1, 2} at center-of-mass energies from 4.009 to 4.360 GeV"

    No full text
    The results on e+e−→γχc2e^+e^-\to\gamma\chi_{c2} Born cross section measurement. Shown in the table are the significance σ\sigma, detection efficiency ϵ\epsilon, number of signal events from the fits Nobs^{\rm obs}, radiative correction factor (1+δr1+\delta^{r}), vacuum polarization factor (1+δv1+\delta^{v}), upper limit (at the 90%\% C.L.) on the number of signal events NUP^{\rm UP}, Born cross section σB\sigma^{B} and upper limit (at the 90%\% C.L.) on the Born cross section σUP\sigma^{\rm UP} at different CME points

    "Table 1" of "Evidence for e+e−→γχc1,2e^+e^-\to\gamma\chi_{c1, 2} at center-of-mass energies from 4.009 to 4.360 GeV"

    No full text
    The results on e+e−→γχc0e^+e^-\to\gamma\chi_{c0} Born cross section measurement. Shown in the table are the significance σ\sigma, detection efficiency ϵ\epsilon, number of signal events from the fits Nobs^{\rm obs}, radiative correction factor (1+δr1+\delta^{r}), vacuum polarization factor (1+δv1+\delta^{v}), upper limit (at the 90%\% C.L.) on the number of signal events NUP^{\rm UP}, Born cross section σB\sigma^{B} and upper limit (at the 90%\% C.L.) on the Born cross section σUP\sigma^{\rm UP} at different CME points. Numbers taken from journal version: some slight differences with respect to arXiv:1411.6336v1 in last two columns

    "Table 2" of "Study of e+e−→ppˉe^+e^- \rightarrow p\bar{p} in the vicinity of ψ(3770)\psi(3770)"

    No full text
    The two solutions of the dressed cross section and the corresponding phase angles, PHI

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

    No full text
    Bare cross section σbare(e+e−→π+π−(γFSR))\sigma^\mathrm{bare}(e^+e^-\to\pi^+\pi^-(\gamma_\mathrm{FSR})) of the process e+e−→π+π−e^+e^-\to\pi^+\pi^- measured using the initial state radiation method. The data is corrected concerning final state radiation and vacuum polarization effects. The final state radiation is added using the Schwinger term at born level

    "Covariance Matrix of the Pion Form Factor" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

    No full text
    Statistical covariance matrix of the pion form factor ∣Fπ∣2|F_\pi|^2

    "Pion Form Factor" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

    No full text
    Pion form factor ∣Fπ∣2|F_\pi|^2 measured using the initial state radiation method. The data is corrected concerning vacuum polarization effects

    "Table 1" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

    No full text
    Results for the bare cross section σπ+π−bare\sigma^\text{bare}_{\pi^+\pi^-} and the pion form factor together with their statistical uncertainties. The systematical uncertainties are given by 0.9% (see arXiv:1507.08188)
    corecore