379 research outputs found

    Search for tetraquark states XccsˉsˉX_{cc\bar{s}\bar{s}} in Ds+Ds+ (Ds+Ds+)D_{s}^{+}D_{s}^{+}~(D_{s}^{*+}D_{s}^{*+}) final states at Belle

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    A search for double-heavy tetraquark state candidates XccsˉsˉX_{cc\bar{s}\bar{s}} decaying to Ds+Ds+D_{s}^{+}D_{s}^{+} and Ds+Ds+D_{s}^{*+} D_{s}^{*+} is presented for the first time using the data samples of 102 million Υ(1S)\Upsilon(1S) and 158 million Υ(2S)\Upsilon(2S) events, and the data samples at s\sqrt{s} = 10.52~GeV, 10.58~GeV, and 10.867~GeV corresponding to integrated luminosities of 89.5~fb1^{-1}, 711.0~fb1^{-1}, and 121.4~fb1^{-1}, respectively, accumulated with the Belle detector at the KEKB asymmetric energy electron-positron collider. The invariant-mass spectra of the Ds+Ds+D_{s}^{+}D_{s}^{+} and Ds+Ds+D_{s}^{*+} D_{s}^{*+} are studied to search for possible resonances. No significant signals are observed, and the 90% confidence level upper limits on the product branching fractions [B(Υ(1S,2S)Xccsˉsˉ+anything)×B(XccsˉsˉDs+Ds+(Ds+Ds+)){\cal B}(\Upsilon(1S,2S) \to X_{cc\bar{s}\bar{s}} + anything) \times {\cal B}(X_{cc\bar{s}\bar{s}} \to D_{s}^{+}D_{s}^{+}(D_{s}^{*+} D_{s}^{*+}))] in Υ(1S,2S)\Upsilon(1S,2S) inclusive decays and the product values of Born cross section and branching fraction [σ(e+eXccsˉsˉ+anything)×B(XccsˉsˉDs+Ds+(Ds+Ds+))\sigma(e^+e^- \to X_{cc\bar{s}\bar{s}} + anything ) \times {\cal B}(X_{cc\bar{s}\bar{s}} \to D_{s}^{+}D_{s}^{+}(D_{s}^{*+} D_{s}^{*+}))] in e+ee^+e^- collisions at s\sqrt{s} = 10.52~GeV, 10.58~GeV, and 10.867~GeV under different assumptions of XccsˉsˉX_{cc\bar{s}\bar{s}} masses and widths are obtained

    Search for Z′ →μ+μ- in the Lμ-Lτ gauge-symmetric model at Belle

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    We search for a new gauge boson Z′ that couples only to heavy leptons and their corresponding neutrinos in the process e+e-→Z′(→μ+μ-)μ+μ-, using a 643 fb-1 data sample collected by the Belle experiment at or near the Υ(1S,2S,3S,4S,5S) resonances at the KEKB collider. While previous searches for Z′ performed a data-based estimation of the initial state radiation effect, our search for the Z′ is the first to include effects due to initial state radiation in the signal simulated samples that were used in estimating the detection efficiency. No signal is observed in the Z′ mass range of 0.212-10 GeV/c2, and we set an upper limit on the coupling strength, g′, constraining the possible Z′ contribution to the anomalous magnetic dipole moment of the muon

    Search for an invisible ZZ^\prime in a final state with two muons and missing energy at Belle II

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    The LμLτL_{\mu}-L_{\tau} extension of the standard model predicts the existence of a lepton-flavor-universality-violating ZZ^{\prime} boson that couples only to the heavier lepton families. We search for such a ZZ^\prime through its invisible decay in the process e+eμ+μZe^+ e^- \to \mu^+ \mu^- Z^{\prime}. We use a sample of electron-positron collisions at a center-of-mass energy of 10.58GeV collected by the Belle II experiment in 2019-2020, corresponding to an integrated luminosity of 79.7fb1^{-1}. We find no excess over the expected standard-model background. We set 90%\%-confidence-level upper limits on the cross section for this process as well as on the coupling of the model, which ranges from 3×1033 \times 10^{-3} at low ZZ^{\prime} masses to 1 at ZZ^{\prime} masses of 8GeV/c2GeV/c^{2}

    Search for Zμ+μZ^{'} \rightarrow \mu^{+} \mu^{-} in the LμLτL_\mu {-} L_\tau gauge-symmetric model at Belle

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    We search for a new gauge boson ZZ' that couples only to heavy leptons and their corresponding neutrinos in the process e+eZ(μ+μ)μ+μe^{+} e^{-} \rightarrow Z'(\rightarrow \mu^{+}\mu^{-}) \mu^{+}\mu^{-}, using a 643 fb1^{-1} data sample collected by the Belle experiment at or near the Υ(1S,2S,3S,4S,5S)\Upsilon(1S,2S,3S,4S,5S) resonances at the KEKB collider. For the first time, effects due to initial state radiation are used in estimating the detection efficiency. No signal is observed in the mass range of 0.212100.212-10 GeV/c2GeV/c^2 and we set an upper limit on the coupling strengh, gg', constraining ZZ' as a possible contributor to the anomalous magnetic dipole moment of muon

    Search for tetraquark states Xcc s- s- in Ds+ Ds+ (Ds∗+ Ds∗+) final states at Belle

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    A search for double-heavy tetraquark state candidates Xccs ̄s ̄ decaying to Ds+Ds+ and Ds∗+Ds∗+ is presented for the first time using the data samples of 102×106 Υ(1S) and 158×106 Υ(2S) events, and the data samples at s=10.52, 10.58, and 10.867 GeV corresponding to integrated luminosities of 89.5, 711.0, and 121.4 fb-1, respectively, accumulated with the Belle detector at the KEKB asymmetric energy electron-positron collider. The invariant-mass spectra of the Ds+Ds+ and Ds∗+Ds∗+ are studied to search for possible resonances. No significant signals are observed, and the 90% confidence level upper limits on the product branching fractions [B(Υ(1S,2S)→Xccs ̄s ̄+anything)×B(Xccs ̄s ̄→Ds+Ds+(Ds∗+Ds∗+))] in Υ(1S,2S) inclusive decays and the product values of Born cross section and branching fraction [σ(e+e-→Xccs ̄s ̄+anything)×B(Xccs ̄s ̄→Ds+Ds+(Ds∗+Ds∗+))] in e+e- collisions at s=10.52, 10.58, and 10.867 GeV under different assumptions of Xccs ̄s ̄ masses and widths are obtained

    Search for an invisibly decaying ZprimeZ^prime boson at Belle II in e+eoμ+μ(epmμmp)e^+ e^- o μ^+ μ^- (e^pm μ^mp) plus missing energy final states

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    Using data collected by the Belle II experiment during 2018 at the SuperKEKB collider, we perform the first searches for the invisible decay of a ZprimeZ^prime in the process e+eomu+muZprimee^+ e^- o mu^+ mu^- Z^prime and of a lepton-flavor-violating ZprimeZ^prime in e+eoepmmumpZprimee^+ e^- o e^pm mu^mp Z^prime. We do not find any excess of events and set 90% credibility level upper limits on the cross sections of these processes. We translate the former, in the framework of an LmuLauL_mu-L_ au theory, into upper limits on the ZprimeZ^prime coupling constant at the level of 5imes102div15 imes 10^-2div1 for MZprimeleq6M_Z^primeleq 6 GeV/c2c^2

    Study of e+e- → D (1 S,2 S)η and e+e- → D (1S)η′ at s =10.866 GeV with the Belle detector

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    We report the first observation of the processes e+e-→D(1S,2S)η at s=10.866 GeV, with significance exceeding 10σ for both processes. The measured Born cross sections are σ(e+e-→D(2S)η)=2.07±0.21±0.19 pb, and σ(e+e-→D(1S)η)=0.42±0.08±0.04 pb. We also set the upper limit on the cross section of the process e+e-→D(1S)η′ to be σ(e+e-→D(1S)η′)<0.037 pb at 90% C.L. The results are obtained with the data sample collected with the Belle detector at the KEKB asymmetric-energy e+e- collider in the energy range from 10.63 to 11.02 GeV

    Measurement of the branching fractions for Cabibbo-suppressed decays D+→K+K−π+π0 and D(s)+→K+π−π+π0 at Belle

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    We present measurements of the branching fractions for the singly Cabibbo-suppressed decays D+→K+K−π+π0 and D+s→K+π−π+π0, and the doubly Cabibbo-suppressed decay D+→K+π−π+π0, based on 980 fb−1 of data recorded by the Belle experiment at the KEKB e+e− collider. We measure these modes relative to the Cabibbo-favored modes D+→K−π+π+π0 and D+s→K+K−π+π0. Our results for the ratios of branching fractions are B(D+→K+K−π+π0)/B(D+→K−π+π+π0)=(11.32±0.13±0.26)%, B(D+→K+π−π+π0)/B(D+→K−π+π+π0)=(1.68±0.11±0.03)%, and B(D+s→K+π−π+π0)/B(D+s→K+K−π+π0)=(17.13±0.62±0.51)%, where the uncertainties are statistical and systematic, respectively. The second value corresponds to (5.83±0.42)×tan4θC, where θC is the Cabibbo angle; this value is larger than other measured ratios of branching fractions for a doubly Cabibbo-suppressed charm decay to a Cabibbo-favored decay. Multiplying these results by world average values for B(D+→K−π+π+π0) and B(D+s→K+K−π+π0) yields B(D+→K+K−π+π0)=(7.08±0.08±0.16±0.20)×10^−3, B(D+→K+π−π+π0)=(1.05±0.07±0.02±0.03)×10^−3, and B(D+s→K+π−π+π0)=(9.44±0.34±0.28±0.32)×10^−3, where the third uncertainty is due to the branching fraction of the normalization mode. The first two results are consistent with, but more precise than, the current world averages. The last result is the first measurement of this branching fraction

    Search for rare decays B+Ds()+ηB^{+} \to D_{s}^{(\ast)+}\eta, Ds()+Kˉ0D_{s}^{(\ast)+}\bar{K}^{0}, D+ηD^{+}\eta, and D+K0D^{+}K^{0}

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    7 pages, 2 figuresInternational audienceWe present a study of rare decay modes B+Ds+h0B^{+} \to D_{s}^{+}h^{0}, B+Ds+h0B^{+} \to D_{s}^{\ast+}h^{0}, and B+D+h0B^{+} \to D^{+}h^{0}, where h0h^{0} denotes the neutral mesons η\eta or K0K^{0}, using a data sample of (772±10)×106(772 \pm 10 ) \times 10^{6} BBˉB\bar{B} events produced at the Υ(4S)\Upsilon(4S) resonance. The data were collected by the Belle detector operating at the asymmetric-energy KEKB collider. We observe no evidence for these decays, so we provide upper limits at the 90%\% confidence level on the branching fractions of B+Ds+h0B^{+} \to D_{s}^{+}h^{0}, Ds+h0D_{s}^{\ast+}h^{0}, and D+h0D^{+}h^{0} decay modes. Along with rare decay modes, we report improved measurements of the color-suppressed decay branching fractions B(Bˉ0D0η)\mathcal{B}(\bar{B}^{0} \to D^{0}\eta) = (26.6 ±\pm 1.2 ±\pm 2.1) ×\times 10510^{-5} and B(Bˉ0D0Kˉ0)\mathcal{B}(\bar{B}^{0} \to D^{0}\bar{K}^{0}) = (5.6 ±\pm 0.5 ±\pm 0.2) ×\times 10510^{-5}. The first and second uncertainties are statistical and systematic, respectively

    Observation of charmed strange meson pair production in Y(2S) decays and in e+e− annihilation at sqrt(s)=10.52 GeV

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    We observe the process Y(2S)→D(*)+s D−sJ and continuum production e+e-→D(*)+s D-sJ at sqrt(s)=10.52 GeV (and their charge conjugates) using the data samples collected by the Belle detector at KEKB, where D-sJ is Ds1(2536)− or D*s2(2573)−. Both D-sJ states are identified through their decay into KD(*). We measure the products of branching fractions B(Y(2S)→D(*)+s D−sJ)B(D-sJ→KD(*)) and the Born cross sections σBorn(e+e-→D(*)+s D-sJ)B(D-sJ→KD(*)), and then compare the ratios R1=B(Y(2S)→D(*)+s D−sJ)/B(Y(2S)→μ+μ−) for Y(2S) decays and R1=σBorn(e+e-→D(*)+s D-sJ)/σBorn(e+e-→μ+μ−) for continuum production. We obtain R1/R2=9.7±2.3±1.1, 6.8±2.1±0.8, 10.2±3.3±2.5, and 3.4±2.1±0.8 for the D+s Ds1(2536)−, D*+s Ds1(2536)−, D+s D*s2(2573)−, and D*+s D*s2(2573)− final states in the D-sJ→K−D(*)0 modes, respectively. The measured R1/R2 values indicate that the strong decay dominates in Y(2S)→D(*)+s D−sJ processes. We also measure the ratios of branching fractions B(Ds1(2536)−→K0SD*(2010)−)/B(Ds1(2536)−→K-D*(2007)0)=0.48±0.07±0.02 and B(D*s2(2573)−→K0SD-)/B(D*s2(2573)−→K-D0)=0.49±0.10±0.02, which are consistent with isospin symmetry. The second ratio is the first measurement of this quantity. Here, the first uncertainties are statistical and the second are systematic
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