463 research outputs found

    Search for the decay J/ψ→γ+invisibleJ/\psi\to\gamma + \rm {invisible}

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    We search for J/ψJ/\psi radiative decays into a weakly interacting neutral particle, namely an invisible particle, using the J/ψJ/\psi produced through the process ψ(3686)→π+π−J/ψ\psi(3686)\to\pi^+\pi^-J/\psi in a data sample of (448.1±2.9)×106(448.1\pm2.9)\times 10^6 ψ(3686)\psi(3686) decays collected by the BESIII detector at BEPCII. No significant signal is observed. Using a modified frequentist method, upper limits on the branching fractions are set under different assumptions of invisible particle masses up to 1.2  GeV/c2\mathrm{\ Ge\kern -0.1em V}/c^2. The upper limit corresponding to an invisible particle with zero mass is 7.0×10−7\times 10^{-7} at the 90\% confidence level

    Search for the reaction e+e−→χcJπ+π− and a charmoniumlike structure decaying to χcJπ± between 4.18 and 4.60 GeV

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    We search for the process e+e-→χcJπ+π- (J=0, 1, 2) and for a charged charmoniumlike state in the χcJπ± subsystem. The search uses datasets collected with the BESIII detector at the BEPCII storage ring at center-of-mass energies between 4.18 GeV and 4.60 GeV. No significant χcJπ+π- signals are observed at any center-of-mass energy, and thus upper limits are provided which also serve as limits for a possible charmoniumlike structure in the invariant χcJπ± mass

    Observation of a structure in e+e−→ϕη′e^+e^- \to \phi \eta^{\prime} at s\sqrt{s} from 2.05 to 3.08 GeV

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    The process e+e−→ϕη′e^{+}e^{-} \to \phi \eta^{\prime} has been studied for the first time in detail using data sample collected with the BESIII detector at the BEPCII collider at center of mass energies from 2.05 to 3.08 GeV. A resonance with quantum numbers JPC=1−−J^{PC}=1^{--} is observed with mass MM = (2177.5 ±\pm 4.8 (stat) ±\pm 19.5 (syst)) MeV/c2{ \it{c}^{\mathrm{2}}} and width Γ\Gamma = (149.0 ±\pm 15.6 (stat) ±\pm 8.9 (syst)) MeV with a statistical significance larger than 10σ\sigma. The observed structure could be identified with the ϕ(2170)\phi(2170), then the ratio of partial width between the ϕη′\phi \eta^{\prime} by BESIII and ϕη\phi \eta by BABAR is (BϕηRΓeeR)/(Bϕη′RΓeeR)\mathcal{B}^{R}_{\phi \eta}\Gamma^{R}_{ee})/{(\mathcal{B}^{R}_{\phi \eta^{\prime}}\Gamma^{R}_{ee})} = 0.23 ±\pm 0.10 (stat) ±\pm 0.18 (syst), which is smaller than the prediction of the ssˉgs\bar{s}g hybrid models by several orders of magnitude

    Search for Λˉ\bar{\Lambda}-Λ\Lambda oscillations in the decay J/ψ→pK−Λˉ+c.c.J/\psi \to p K^- \bar{\Lambda}+c.c.

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    We report the first search for Λˉ\bar\Lambda--Λ\Lambda oscillations in the decay J/ψ→pK−Λˉ+c.c.J/\psi \to p K^- \bar{\Lambda} + c.c. by analyzing 1.31×1091.31\times10^9 J/ψJ/\psi events accumulated with the BESIII detector at the BEPCII collider. The J/ψJ/\psi events are produced using e+e−e^+e^- collisions at a center of mass energy s=3.097\sqrt{s}= 3.097~GeV. No evidence for hyperon oscillations is observed. The upper limit for the oscillation rate of Λˉ\bar\Lambda to Λ\Lambda hyperons is determined to be P(Λ)=B(J/ψ→pK−Λ+c.c.)B(J/ψ→pK−Λˉ+c.c.)<4.4×10−6\mathcal{P}(\Lambda)=\frac{\mathcal{B}(J/\psi\to pK^-\Lambda+c.c.)}{\mathcal{B}(J/\psi\to pK^-\bar\Lambda+c.c.)}<4.4\times10^{-6} corresponding to an oscillation parameter δmΛΛˉ\delta m_{\Lambda\bar\Lambda} of less than 3.8×10−183.8\times10^{-18}~GeV at the 90\% confidence level.Comment: 7 pages, 1 figur

    Amplitude analysis of Ds+→π+π−π+D_s^{+} \rightarrow \pi^{+} \pi^{-} \pi^{+}

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    Utilizing the data set corresponding to an integrated luminosity of 3.193.19 fb−1^{-1} collected by the BESIII detector at a center-of-mass energy of 4.178 GeV, we perform an amplitude analysis of the Ds+→π+π−π+D_s^+\to\pi^+\pi^-\pi^+ decay. The sample contains 13,797 candidates with a signal purity of ∼\sim80%. The amplitude and phase of the contributing ππ\pi\pi S{\cal S} wave are measured based on a quasi-model-independent approach, along with the amplitudes and phases of the P{\cal P} and D{\cal D} waves parametrized by Breit-Wigner models. The fit fractions of different intermediate decay channels are also reported.Comment: 14 pages, 6 figure

    Measurements of the absolute branching fractions of D0(+)→KKˉππD^{0(+)}\to K\bar K\pi\pi decays

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    Based on 2.93~fb−1^{-1} e+e−e^+e^- collision data taken at center-of-mass energy of 3.773 GeV by the BESIII detector, we report the measurements of the absolute branching fractions of D0→K+K−π0π0D^0\to K^+K^-\pi^0\pi^0, D0→KS0KS0π+π−D^0\to K^0_SK^0_S\pi^+\pi^-, D0→KS0K−π+π0D^0\to K^0_SK^-\pi^+\pi^0, D0→KS0K+π−π0D^0\to K^0_SK^+\pi^-\pi^0, D+→K+K−π+π0D^+\to K^+K^-\pi^+\pi^0, D+→KS0K+π0π0D^+\to K^0_SK^+\pi^0\pi^0, D+→KS0K−π+π+D^+\to K^0_SK^-\pi^+\pi^+, D+→KS0K+π+π−D^+\to K^0_SK^+\pi^+\pi^-, and D+→KS0KS0π+π0D^+\to K^0_SK^0_S\pi^+\pi^0. The decays D0→K+K−π0π0D^0\to K^+K^-\pi^0\pi^0, D0→KS0K−π+π0D^0\to K^0_SK^-\pi^+\pi^0, D0→KS0K+π−π0D^0\to K^0_SK^+\pi^-\pi^0, D+→KS0KS0π+π0D^+\to K^0_SK^0_S\pi^+\pi^0, and D+→KS0K+π0π0D^+\to K^0_SK^+\pi^0\pi^0 are observed for the first time. The branching fractions of the decays D0→KS0KS0π+π−D^0\to K^0_SK^0_S\pi^+\pi^-, D+→K+K−π+π0D^+\to K^+K^-\pi^+\pi^0, D+→KS0K−π+π+D^+\to K^0_SK^-\pi^+\pi^+, and D+→KS0K+π+π−D^+\to K^0_SK^+\pi^+\pi^- are measured with improved precision compared to the world-average values.Comment: 11 pages, 5 figure
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