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  1. Search for the isospin-violating decays χ c J Λ Σ ¯ 0 + c . c . and η c Λ Σ ¯ 0 + c . c .

    Using a sample of ( 2712.4 ± 14.3 ) × 10 6     ψ ( 3686 ) events collected with the BESIII detector, we perform a search for the isospin-violating decays χ c J → Λ Σ ¯   0 + c . c . ( J = 0 , 1 , 2 ) and η c → Λ Σ ¯   0 + c . c . No significant signal for χ c J or η c is observed in the Λ Σ ¯   0 invariant mass distribution. The upper limits on the branching fractions at the 90% confidencemore » level are set to be B ( χ c 0 → Λ Σ ¯   0 + c . c . ) < 1.5 × 10 − 6 , B ( χ c 1 → Λ Σ ¯   0 + c . c . ) < 1.6 × 10 − 6 , B ( χ c 2 → Λ Σ ¯   0 + c . c . ) < 1.7 × 10 − 6 , and B ( η c → Λ Σ ¯   0 + c . c . ) < 6.2 × 10 − 5 for the first time.« less
  2. Search for the lepton-flavor-violating τ → e± decays at Belle II

    We present the result of a search for the charged-lepton-flavor violating decays τ → e±, where ℓ is a muon or an electron, using a data sample with an integrated luminosity of 428 fb−1 recorded by the Belle II experiment at the SuperKEKB e+e collider. The selection of e+e → τ+τ events containing a signal candidate is based on an inclusive-tagging reconstruction and on a boosted decision tree to suppress background. Upper limits on the branching fractions between 1.3 and 2.5 × 10−8 are set at the 90% confidence level. These results are the most stringent bounds to date formore » four of the modes.« less
  3. Search for an axion-like particle in B → K(*)a(→ γγ) decays at Belle

    We report a search for an axion-like particle a in B → K(*)a decays using data collected with the Belle detector at the KEKB asymmetric-energy electron-positron collider. The search is based on a 711 fb−1 data sample collected at the Υ(4S) resonance energy, corresponding to a sample of 772 × 106 Υ(4S) events. In this study, we search for the decay of the axion-like particle into a pair of photons, a → γγ. We scan the two-photon invariant mass in the range 0.16 GeV–4.50 GeV for the K modes and 0.16 GeV–4.20 GeV for the K* modes. No significant signalmore » is observed in any of the modes, and 90% confidence level upper limits are established on the coupling to the W boson, gaW, as a function of a mass. The limits range from 3 × 10−6 GeV−1 to 3 × 10−5 GeV−1, improving the current constraints on gaW by a factor of two over the most stringent previous experimental results.« less
  4. Model-agnostic likelihood for the reinterpretation of the 𝐵+→ 𝐾+⁢$$𝑣\bar{𝑣}$$ measurement at Belle II

    We recently measured the branching fraction of the 𝐵+→ 𝐾+⁢$$𝑣\bar{𝑣}$$ decay using 362 fb−1 of on-resonance 𝑒+⁢𝑒 collision data under the assumption of Standard Model kinematics, providing the first evidence for this decay. To facilitate future reinterpretations and maximize the scientific impact of this measurement, we publicly release the full analysis likelihood along with all necessary material required for reinterpretation under arbitrary theoretical models sensitive to this measurement. In this work, we demonstrate how the measurement can be reinterpreted within the framework of the weak effective theory. Using a kinematic reweighting technique in combination with the published likelihood, we derivemore » marginal posterior distributions for the Wilson coefficients, construct credible intervals, and assess the goodness of fit to the Belle II data. For the weak effective theory Wilson coefficients, the posterior mode of the magnitudes |𝐶VL+𝐶VR|, |𝐶SL +𝐶SR|, and |𝐶TL| corresponds to the point (11.3, 0.0, 8.2). The respective 95% credible intervals are [1.9, 16.2], [0.0, 15.4], and [0.0, 11.2].« less
  5. Measurement of the phase between strong and electromagnetic amplitudes in the decay J/ψ → ϕη

    The first direct measurement of the relative phase between the strong and electromagnetic amplitudes for a J/ψ decaying into a vector-pseudoscalar final state is performed using 26 energy points of e+e annihilation data between 3.00 GeV and 3.12 GeV. The data sets were collected by the BESIII detector with a total integrated luminosity of 452 pb−1. By investigating the interference pattern in the cross section lineshape of e+e → ϕη, the relative phase between the strong and electromagnetic amplitudes of J/ψ decay is determined to be within [133°, 228°] at 68% confidence level.
  6. Charged-hadron identification at Belle II

    The Belle II experiment’s ability to identify particles critically affects the sensitivity of its measurements. We describe Belle II’s algorithms for identifying charged particles and evaluate their performance in separating pions, kaons, and protons using $$426\,\text {fb}^{-1}$$ of data collected at the energy-asymmetric $$e^{+}e^{-}$$ collider SuperKEKB in 2019–2022 at center-of-mass energies at and near the mass of the $$\Upsilon$$ (4S).
  7. Measurement of the 𝐷0→𝐾⁢𝜋+⁢𝑒+⁢𝑒 branching fraction and search for 𝐷0 → 𝜋+⁢𝜋⁢𝑒+⁢𝑒 and 𝐷0 →𝐾+⁢𝐾⁢𝑒+⁢𝑒 decays at Belle

    We present a study of the rare charm meson decays 𝐷0 →𝐾+⁢𝐾⁢𝑒+⁢𝑒, 𝜋+⁢𝜋⁢𝑒+⁢𝑒, and 𝐾⁢𝜋+⁢𝑒+⁢𝑒 using a 942  fb−1 dataset collected by the Belle detector at the KEKB asymmetric-energy 𝑒+⁢𝑒 collider. We identify 𝐷0 candidates via the charge of the pion from 𝐷*+ →𝐷0⁢𝜋+ decays and normalize the branching fractions to 𝐷0 → 𝐾⁢𝜋+⁢𝜋⁢𝜋+ decays. The branching fraction for decay 𝐷0 → 𝐾⁢𝜋+⁢𝑒+⁢𝑒 is measured to be (39.6 ± 4.5 (stat) ± 2.9 (syst)) × 10−7, with the dielectron mass in the 𝜌/𝜔 mass region 675 < 𝑚𝑒⁢𝑒 < 875  MeV/⁢𝑐2. We also search for 𝐷0 → ℎ⁡ℎ(′)+⁡𝑒+⁢𝑒 (ℎ(′) = 𝐾, 𝜋) decays withmore » the dielectron mass near the 𝜂 and 𝜙 resonances, and away from these resonances for the 𝐾+⁢𝐾⁢𝑒+⁢𝑒 and 𝜋+⁢𝜋⁢𝑒+⁢𝑒 modes. For these modes, we find no significant signals and set 90% confidence level upper limits on their branching fractions at the 𝒪⁡(10−7) level.« less
  8. Search for B0 → K*0𝜏+⁢𝜏 Decays at the Belle II Experiment

    We present a search for the rare flavor-changing neutral-current decay 𝐵0→𝐾*0⁢𝜏+⁢𝜏 with data collected by the Belle II experiment at the SuperKEKB electron-positron collider. The analysis uses a 365 fb−1 data sample recorded at the center-of-mass energy of the ϒ⁡(4⁢𝑆) resonance. One of the 𝐵 mesons produced in the ϒ⁡(4⁢𝑆)→𝐵0$$⁢\overline{𝐵}$$0 process is fully reconstructed in a hadronic decay mode, while its companion 𝐵 meson is required to decay into a 𝐾*0 and two 𝜏 leptons of opposite charge. The 𝜏 leptons are reconstructed in final states with a single electron, muon, charged pion or charged 𝜌 meson, and additional neutrinos.more » We set an upper limit on the branching fraction of ℬ⁡(𝐵0→𝐾*0⁢𝜏+⁢𝜏)<1.8×10−3 at the 90% confidence level, which is the most stringent constraint reported to date.« less
  9. Measurement of 𝐵+ →𝜏+⁢𝜈𝜏 branching fraction with a hadronic tagging method at Belle II

    We present a measurement of the branching fraction of 𝐵+ →𝜏+⁢𝜈𝜏 decays using 387±6×106 ϒ⁡(4⁢𝑆) collected between 2019 and 2022 with the Belle II detector at the SuperKEKB 𝑒+⁢𝑒 collider. We reconstruct the accompanying 𝐵 meson using the hadronic tagging method, while 𝐵+ →𝜏+⁢𝜈𝜏 candidates are identified in the recoil. We find evidence for 𝐵+ →𝜏+⁢𝜈𝜏 decays at 3.0 standard deviations, including systematic uncertainties. The measured branching fraction is ℬ⁡(𝐵+ →𝜏+⁢𝜈𝜏)=[1.24±0.41⁢(stat)±0.19⁢(syst)]×10−4.
  10. Search for a Dark Higgs Boson Produced in Association with Inelastic Dark Matter at the Belle II Experiment

    Inelastic dark matter models that have two dark matter particles and a massive dark photon can reproduce the observed relic dark matter density without violating cosmological limits. The mass splitting between the two dark matter particles 𝜒1 and 𝜒2, with 𝑚⁡(𝜒2) >𝑚⁡(𝜒1), is induced by a dark Higgs field and a corresponding dark Higgs boson ℎ′. We present a search for dark matter in events with two vertices, at least one of which must be displaced from the interaction region, and missing energy. Using a 365 fb−1 data sample collected at Belle II, which operates at the SuperKEKB 𝑒+⁢𝑒 collider,more » we observe no evidence for a signal. We set upper limits on the product of the production cross section 𝜎⁡(𝑒+⁢𝑒 → ℎ′⁡𝜒1⁢𝜒2), and the product of branching fractions ℬ⁡(𝜒2 → 𝜒1⁢𝑒+⁢𝑒) ×ℬ⁡(ℎ′ → 𝑥+⁢𝑥), where 𝑥+⁢𝑥 indicates 𝜇+⁢𝜇, 𝜋+⁢𝜋, or 𝐾+⁢𝐾, as functions of ℎ′ mass and lifetime at the level of 10−1 fb. We set model-dependent upper limits on the dark Higgs mixing angle at the level of 10−5 and on the dark photon kinetic mixing parameter at the level of 10−3. This is the first search for dark Higgs bosons in association with inelastic dark matter.« less
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