712 research outputs found

    Studies of Charmonium at BESIII

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    Based on ψ(3686)\psi(3686) decays of 106 million, the 1.31 billion J/psi events and a data sample of ψ(3770)\psi(3770) with 2.9 fb−12.9~fb^{-1} integrated luminosity, many analyses are performed. Exclusively baryonic decays of the ψ(3770)\psi(3770), the radiative transition ψ(3770)→γηc(2S)\psi(3770)\to\gamma\eta_c(2S), the ψ(3770)\psi(3770) transition to χcJ\chi_{cJ}, isospin violation decay χc0,2→π0ηc\chi_{c0,2}\to\pi^0\eta_c, the C−C-parity violation decays J/ψ→γγ,γϕJ/\psi\to\gamma\gamma,\gamma\phi are searched for, but no significant signals are observed, and upper limits are set for these decays. The decays of ψ(3770)→γχc1\psi(3770)\to\gamma\chi_{c1} and J/ψ→π0ϕJ/\psi\to\pi^0\phi signals are observed. These measurements provide more information on the charmonium structure, and the isospin and CC-parity violation in the charmonium decays.Comment: 8 pages, 4 figures, to be published in the proceedings of CHARM-2015, Detroit, MI, 18-22 May 201

    Observation of Zc(3900)0Z_c(3900)^{0} in e+e−→π0π0J/ψe^+e^-\to\pi^0\pi^0 J/\psi

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    Using a data sample collected with the BESIII detector operating at the BEPCII storage ring, we observe a new neutral state Zc(3900)0Z_c(3900)^{0} with a significance of 10.4σ10.4\sigma. The mass and width are measured to be 3894.8±2.3±3.23894.8\pm2.3\pm3.2 MeV/c2c^2 and 29.6±8.2±8.229.6\pm8.2\pm8.2~MeV, respectively, where the first error is statistical and the second systematic. The Born cross section for e+e−→π0π0J/ψe^+e^-\to\pi^0\pi^0 J/\psi and the fraction of it attributable to π0Zc(3900)0→π0π0J/ψ\pi^0 Z_c(3900)^{0}\to\pi^0\pi^0 J/\psi in the range Ecm=4.19−4.42E_{cm}=4.19-4.42 GeV are also determined. We interpret this state as the neutral partner of the four-quark candidate Zc(3900)±Z_c(3900)^\pm.Comment: 7 pages, 4 figures, submit to Physics Review Lette

    Measurements of Absolute Branching Fractions of Fourteen Exclusive Hadronic DD Decays to η\eta

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    Using 2.93 fb−12.93\,\rm fb^{-1} of e+e−e^+e^- collision data taken at a center-of-mass energy of 3.773\,GeV with the BESIII detector, we report the first measurements of the absolute branching fractions of fourteen hadronic D0(+)D^{0(+)} decays to exclusive final states with an η\eta, e.g., D0→K−π+ηD^0\to K^-\pi^+\eta, KS0π0ηK^0_S\pi^0\eta, K+K−ηK^+K^-\eta, KS0KS0ηK^0_SK^0_S\eta, K−π+π0ηK^-\pi^+\pi^0\eta, KS0π+π−ηK^0_S\pi^+\pi^-\eta, KS0π0π0ηK^0_S\pi^0\pi^0\eta, and π+π−π0η\pi^+\pi^-\pi^0\eta; D+→KS0π+ηD^+\to K^0_S\pi^+\eta, KS0K+ηK^0_SK^+\eta, K−π+π+ηK^-\pi^+\pi^+\eta, KS0π+π0ηK^0_S\pi^+\pi^0\eta, π+π+π−η\pi^+\pi^+\pi^-\eta, and π+π0π0η\pi^+\pi^0\pi^0\eta. Among these decays, the D0→K−π+ηD^0\to K^-\pi^+\eta and D+→KS0π+ηD^+\to K^0_S\pi^+\eta decays have the largest branching fractions, which are B(D0→K−π+η)=(1.853±0.025stat±0.031syst)%\mathcal{B} (D^0\to K^-\pi^+\eta )=(1.853\pm0.025_{\rm stat}\pm0.031_{\rm syst})\% and B(D+→KS0π+η)=(1.309±0.037stat±0.031syst)%\mathcal{B}(D^+\to K^0_S\pi^+\eta)=(1.309\pm0.037_{\rm stat}\pm0.031_{\rm syst})\%, respectively. We also determine the CPCP asymmetries for the six decays with highest event yields. No evidence of CPCP violation is found.Comment: 11 pages, 3 figure

    Study of charmonium decays at BESIII

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    Based on the data samples collected at the energies of J/ψJ/\psi, ψ(3686)\psi(3686), ψ(3770)\psi(3770) and ψ(4040)\psi(4040) resonances with the BESIII detector at the BEPCII storage ring, we present charmonium decays in two aspects. One is the search for baryonic decays of ψ(3770)\psi(3770) and ψ(4040)\psi(4040), including ΛΛˉπ+π−\Lambda \bar\Lambda\pi^+\pi^-, ΛΛˉπ0\Lambda\bar\Lambda\pi^0, ΛΛˉη\Lambda \bar\Lambda\eta, Σ+Σˉ−\Sigma^+ \bar\Sigma^-, Σ0Σˉ0\Sigma^0 \bar\Sigma^0, Ξ−Ξˉ+\Xi^-\bar\Xi^+ and Ξ0Ξˉ0\Xi^0\bar\Xi^0. None are observed, and upper limits are set at the 90% confidence level. The other is the light hadron spectroscopy from charmonium radiative decays, including the spin-parity analysis of the ppˉp\bar p mass-threshold enhancement in J/ψJ/\psi radiative decays and the ηη\eta\eta system in J/ψ→γηηJ/\psi\to\gamma\eta\eta radiative decays.Comment: to appear in the proceedings of The 6th International Workshop on Charm Physics (CHARM 2013

    Study of the process e+e−→π0π0J/ψe^+e^-\to\pi^0\pi^0 J/\psi and neutral charmonium-like state Zc(3900)0Z_c(3900)^0

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    Cross sections of the process e+e−→π0π0J/ψe^+e^-\to\pi^0\pi^0 J/\psi at center-of-mass energies between 3.808 and 4.600 GeV are measured with high precision by using 12.4 fb−1fb^{-1} of data samples collected with the BESIII detector operating at the BEPCII collider facility. A fit to the measured energy-dependent cross sections confirms the existence of the charmonium-like state Y(4220)Y(4220). The mass and width of the Y(4220)Y(4220) are determined to be (4220.4±2.4±2.3)(4220.4\pm2.4\pm2.3) MeV/c2{\rm MeV}/c^{2} and (46.2±4.7±2.1)(46.2\pm4.7\pm2.1) MeV, respectively, where the first uncertainties are statistical and the second systematic. The mass and width are consistent with those measured in the process e+e−→π+π−J/ψe^+e^-\to\pi^+\pi^- J/\psi. The neutral charmonium-like state Zc(3900)0Z_c(3900)^0 is observed prominently in the π0J/ψ\pi^0 J/\psi invariant-mass spectrum, and, for the first time, an amplitude analysis is performed to study its properties. The spin-parity of Zc(3900)0Z_c(3900)^0 is determined to be JP=1+J^{P}=1^{+}, and the pole position is (3893.1±2.2±3.0)−i(22.2±2.6±7.0)(3893.1\pm2.2\pm3.0)-i(22.2\pm2.6\pm7.0) MeV/c2{\rm MeV}/c^2, which is consistent with previous studies of electrically charged Zc(3900)±Z_c(3900)^\pm. In addition, cross sections of e+e−→π0Zc(3900)0→π0π0J/ψe^+e^-\to\pi^0 Z_c(3900)^0\to \pi^0\pi^0 J/\psi are extracted, and the corresponding lineshape is found to agree with that of the Y(4220)Y(4220).Comment: 8 pages, 3 figure

    Measurements of the branching fractions for J/psi and psi(2S) -> Lambda Lambdabar pi0 and Lambda Lambdabar eta

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    We report on a study of the isospin-violating and conserving decays of the J/psi and psi(2S) charmonium state to Lambda Lambdabar pi0 and Lambda Lambdabar eta, respectively. The data are based on 225 million J/psi and 106 million psi(2S) events that were collected with the BESIII detector. The most accurate measurement of the branching fraction of the isospin-violating process J/psi ->Lambda Lambdabar pi0 is obtained, and the isospin-conserving processes J/psi ->Lambda Lambdabar eta and psi(2S) ->Lambda Lambdabar eta are observed for the first time. The branching fractions are measured to be B(J/psi ->Lambda Lambdabar pi0) = (3.78+-0.27stat)+-0.29sys)10^-5; B(J/psi ->Lambda Lambdabar eta) = (15.7+-0.79stat+-1.52sys)10^-5 and B(psi(2S) ->Lambda Lambdabar eta)= (2.47+-0.34stat+-0.19sys)10^-5. No significant signal events are observed for psi(2S) ->Lambda Lambdabar pi0 decay resulting in an upper limit of the branching fraction of B(psi(2S) ->Lambda Lambdabar pi0) < 0.29X10^-5 at the 90% confidence level. The two-body decay of J/psi-> Sigma(1385)^0 Lambdabar + c.c. is searched for, and the upper limit is B(J/psi-> Sigma(1385)^0 Lambdabar + c.c.) < 0.81X 10^-5 at the 90% confidence level

    Search for a light CP-odd Higgs boson in the radiative decays of J/psi

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    We search for a light Higgs boson A0A^0 in the fully reconstructed decay chain of J/ψ→γA0J/\psi \rightarrow \gamma A^0, A0→μ+μ−A^0 \rightarrow \mu^+\mu^- using (225.0±2.8)×106(225.0\pm2.8)\times10^6 J/ψJ/\psi events collected by the BESIII experiment. The A0A^0 is a hypothetical CP-odd light Higgs boson predicted by many extensions of the Standard Model including two spin-0 doublets plus an extra singlet. We find no evidence for A0A^0 production and set 90%90\% confidence-level upper limits on the product branching fraction B(J/ψ→γA0)×B(A0→μ+μ−)\mathcal{B}(J/\psi \rightarrow \gamma A^0) \times \mathcal{B}(A^0 \rightarrow \mu^+\mu^-) in the range of (2.8−495.3)×10−8(2.8-495.3)\times 10^{-8} for 0.212≤mA0≤3.00.212 \le m_{A^0} \le 3.0 GeV/c2^2. The new limits are 55 times below our previous results, and the nature of the A0A^0 is constrained to be mostly singlet.Comment: 7 pages, 5 figures, submitted to the Physical Review D (rapid communications

    Determination of the number of J/ψ\psi events with J/ψ\psi \rightarrow decays

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    The number of J/ψJ/\psi events collected with the BESIII detector at the BEPCII from June 12 to July 28, 2009 is determined to be (225.3±2.8)×106(225.3\pm2.8)\times10^{6} using J/ψ→inclusiveJ/\psi \rightarrow inclusive events, where the uncertainty is the systematic error and the statistical one is negligible.Comment: 12 pages, 14 figures; (the paper has been received by the Chinese Physics C.

    Search for the rare decay of ψ(3686)→Λc+p‾e+e−+c.c.\psi(3686) \rightarrow \Lambda_c^+ \overline{p} e^+ e^- + c.c. at BESIII

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    Based on a data sample of (448.1±2.9)×106 ψ(3686)(448.1\pm2.9)\times10^6~\psi(3686) decays collected with the BESIII experiment, a search for the flavor changing neutral current transition ψ(3686)→Λc+p‾e+e−+c.c.\psi(3686)\rightarrow \Lambda_c^+ \overline{p} e^+ e^- + c.c. is performed for the first time. No signal candidates are observed and the upper limit on the branching fraction of ψ(3686)→Λc+p‾e+e−\psi(3686)\rightarrow \Lambda_c^+ \overline{p} e^+ e^- is determined to be 1.7×10−61.7\times10^{-6} at the 90\% confidence level. The result is consistent with expectations from the Standard Model, and no evidence for new physics is found.Comment: 6 pages, 2 figures. Accepted by PR

    First Observation of D+→ημ+νμD^+\to \eta\mu^+\nu_\mu and Measurement of its Decay Dynamics

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    By analyzing a data sample corresponding to an integrated luminosity of 2.93 fb−12.93~\mathrm{fb}^{-1} collected at a center-of-mass energy of 3.773 GeV with the BESIII detector, we measure for the first time the absolute branching fraction of the D+→ημ+νμD^+\to \eta \mu^+\nu_\mu decay to be BD+→ημ+νμ=(10.4±1.0stat±0.5syst)×10−4{\mathcal B}_{D^+\to \eta \mu^+\nu_\mu}=(10.4\pm1.0_{\rm stat}\pm0.5_{\rm syst})\times 10^{-4}. Using the world averaged value of BD+→ηe+νe{\mathcal B}_{D^+\to \eta e^+\nu_e}, the ratio of the two branching fractions is determined to be BD+→ημ+νμ/BD+→ηe+νe=0.91±0.13{\mathcal B}_{D^+\to \eta \mu^+\nu_\mu}/{\mathcal B}_{D^+\to \eta e^+\nu_e}=0.91\pm0.13, which agrees with the theoretical expectation of lepton flavor universality within uncertainty. Here, the uncertainty is the sum in quadrature of the statistical and systematic uncertainties. By studying the differential decay rates in five four-momentum transfer intervals, we obtain the product of the hadronic form factor f+η(0)f^{\eta}_{+}(0) and the c→dc\to d Cabibbo-Kobayashi-Maskawa matrix element ∣Vcd∣|V_{cd}| to be f+η(0)∣Vcd∣=0.087±0.008stat±0.002systf_{+}^\eta (0)|V_{cd}|=0.087\pm0.008_{\rm stat}\pm0.002_{\rm syst}. Taking the input of ∣Vcd∣|V_{cd}| from the global fit in the standard model, we determine f+η(0)=0.39±0.04stat±0.01systf_{+}^\eta (0)=0.39\pm0.04_{\rm stat}\pm0.01_{\rm syst}. On the other hand, using the value of f+η(0)f_+^{\eta}(0) calculated in theory, we find ∣Vcd∣=0.242±0.022stat±0.006syst±0.033theory|V_{cd}|=0.242\pm0.022_{\rm stat}\pm0.006_{\rm syst}\pm0.033_{\rm theory}.Comment: 10 pages, 3 figure
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