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  • Springer Science and Business Media LLC  (14)
  • Ablikim, M.  (14)
  • Zhang, Yan
  • 2020-2024  (14)
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  • Springer Science and Business Media LLC  (14)
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  • 2020-2024  (14)
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  • 1
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2024, No. 5 ( 2024-05-03)
    Abstract: Using 24.1 fb − 1 of e + e − collision data collected with the BESIII detector at the BEPCII collider, the Born cross sections and effective form factors of the $$ {e}^{+}{e}^{-}\to {\Sigma}^{+}{\overline{\Sigma}}^{-} $$ e + e − → Σ + Σ ¯ − reaction are measured. The measurements are performed at center-of-mass energies ranging from 3.510 to 4.951 GeV. No significant evidence for the decay of the charmonium(-like) states, ψ (3770), ψ (4040), ψ (4160), Y (4230), Y (4360), ψ (4415), and Y (4660), into a $$ {\Sigma}^{+}{\overline{\Sigma}}^{-} $$ Σ + Σ ¯ − final state is observed. Consequently, upper limits for the products of the branching fractions and the electronic partial widths at the 90% confidence level are reported for these decays.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2024
    detail.hit.zdb_id: 2027350-2
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  • 2
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2023, No. 9 ( 2023-09-12)
    Abstract: Using 2.93 fb − 1 of e + e − collision data collected with the BESIII detector at the center-of-mass energy 3.773 GeV, we perform the first amplitude analysis of the decay D + → $$ {K}_S^0 $$ K S 0 π + π 0 π 0 and determine the relative magnitudes and phases of different intermediate processes. The absolute branching fraction of D + → $$ {K}_S^0 $$ K S 0 π + π 0 π 0 is measured to be (2.888 ± 0.058 stat . ± 0.069 syst . )%. The dominant intermediate processes are D + → $$ {K}_S^0 $$ K S 0 a 1 (1260) + ( → ρ + π 0 ) and D + → $$ \overline{K} $$ K ¯ *0 ρ + , with branching fractions of (8.66 ± 1.04 stat . ± 1.39 syst . ) × 10 − 3 and (9.70 ± 0.81 stat . ± 0.53 syst . ) × 10 − 3 , respectively.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2023
    detail.hit.zdb_id: 2027350-2
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  • 3
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2023, No. 9 ( 2023-09-19)
    Abstract: Utilizing 7 . 33 fb − 1 of e + e − collision data taken at the center-of-mass energies of 4.128, 4.157, 4.178, 4.189, 4.199, 4.209, 4.219, and 4.226 GeV with the BESIII detector, the branching fraction of the leptonic decay $$ {D}_s^{+} $$ D s + → τ + ν τ via τ + → μ + ν μ $$ \overline{\nu} $$ ν ¯ τ is measured to be $$ {\mathcal{B}}_{D_s^{+}\to {\tau}^{+}{\nu}_{\tau }} $$ B D s + → τ + ν τ = (5 . 37 ± 0 . 17 stat ± 0 . 15 syst )%. Combining this branching fraction with the world averages of the measurements of the masses of τ + and $$ {D}_s^{+} $$ D s + as well as the lifetime of $$ {D}_s^{+} $$ D s + , we extract the product of the decay constant of $$ {D}_s^{+} $$ D s + and the c → s Cabibbo-Kobayashi-Maskawa matrix element to be $$ {f}_{D_s^{+}} $$ f D s + |V cs | = (246 . 7 ± 3 . 9 stat ± 3 . 6 syst ) MeV. Taking |V cs | from a global fit in the standard model we obtain $$ {f}_{D_s^{+}} $$ f D s + = (253 . 4 ± 4 . 0 stat ± 3 . 7 syst ) MeV. Conversely, taking $$ {f}_{D_s^{+}} $$ f D s + from lattice quantum chromodynamics calculations, we obtain |V cs | = 0 . 987 ± 0 . 016 stat ± 0 . 014 syst .
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2023
    detail.hit.zdb_id: 2027350-2
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  • 4
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2023, No. 12 ( 2023-12-04)
    Abstract: Using e + e − collision datasets corresponding to a total integrated luminosity of 21.7 fb − 1 collected with the BESIII detector at the BEPCII collider at center-of-mass energies ranging from 4.009 GeV to 4.951 GeV, the energy-dependent cross sections of $$ {e}^{+}{e}^{-}\to p{K}^{-}\overline{\Lambda}+c.c. $$ e + e − → p K − Λ ¯ + c . c . are measured for the first time. By fitting these energy-dependent cross sections, we search for the excited ψ states ψ (4160) and ψ (4415), and the vector charmonium-like states ψ (4230), ψ (4360), and ψ (4660). No evidence for these is observed and the upper limits on the branching fractions of these states decaying into $$ p{K}^{-}\overline{\Lambda}+c.c. $$ p K − Λ ¯ + c . c . are set at the 90% confidence level.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2023
    detail.hit.zdb_id: 2027350-2
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  • 5
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2023, No. 12 ( 2023-12-12)
    Abstract: The $$ {D}_s^{+}\to {K}^{+}{K}^{-}{\mu}^{+}{\nu}_{\mu } $$ D s + → K + K − μ + ν μ decay is studied based on 7.33 fb − 1 of e + e − collision data collected with the BESIII detector at center-of-mass energies in the range from 4.128 to 4.226 GeV. The absolute branching fraction is measured as $$ \mathcal{B}\left({D}_s^{+}\to \phi {\mu}^{+}{\nu}_{\mu}\right)=\left(2.25\pm 0.09\pm 0.07\right)\times {10}^{-2} $$ B D s + → ϕ μ + ν μ = 2.25 ± 0.09 ± 0.07 × 10 − 2 , the most precise measurement to date. Combining with the world average of $$ \mathcal{B}\left({D}_s^{+}\to \phi {e}^{+}{\nu}_e\right) $$ B D s + → ϕ e + ν e , the ratio of the branching fractions obtained is $$ \frac{\mathcal{B}\left({D}_s^{+}\to \phi {\mu}^{+}{\nu}_{\mu}\right)}{\mathcal{B}\left({D}_s^{+}\to \phi {e}^{+}{\nu}_e\right)}=0.94\pm 0.08 $$ B D s + → ϕ μ + ν μ B D s + → ϕ e + ν e = 0.94 ± 0.08 , in agreement with lepton universality. By performing a partial wave analysis, the hadronic form factor ratios at q 2 = 0 are extracted, finding $$ {r}_V=\frac{V(0)}{A_1(0)}=1.58\pm 0.17\pm 0.02 $$ r V = V 0 A 1 0 = 1.58 ± 0.17 ± 0.02 and $$ {r}_2=\frac{A_2(0)}{A_1(0)}=0.71\pm 0.14\pm 0.02 $$ r 2 = A 2 0 A 1 0 = 0.71 ± 0.14 ± 0.02 , where the first uncertainties are statistical and the second are systematic. No significant S -wave contribution from f 0 (980) → K + K − is found. The upper limit $$ \mathcal{B}\left({D}_s^{+}\to {f}_0(980){\mu}^{+}{\nu}_{\mu}\right)\cdot \mathcal{B}\left({f}_0(980)\to {K}^{+}{K}^{-}\right) 〈 5.45\times {10}^{-4} $$ B D s + → f 0 980 μ + ν μ ⋅ B f 0 980 → K + K − 〈 5.45 × 10 − 4 is set at 90% credibility level.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2023
    detail.hit.zdb_id: 2027350-2
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  • 6
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2023, No. 9 ( 2023-09-19)
    Abstract: Based on 4.5 fb − 1 data taken at seven center-of-mass energies ranging from 4.600 to 4.699 GeV with the BESIII detector at the BEPCII collider, we measure the branching fractions of $$ {\Lambda}_c^{+} $$ Λ c + → Σ + + hadrons relative to $$ {\Lambda}_c^{+} $$ Λ c + → Σ + π + π − . Combining with the world average branching fraction of $$ {\Lambda}_c^{+} $$ Λ c + → Σ + π + π − , their branching fractions are measured to be (0 . 377 ± 0 . 042 ± 0 . 020 ± 0 . 021)% for $$ {\Lambda}_c^{+} $$ Λ c + → Σ + K + K − , (0 . 200 ± 0 . 023 ± 0 . 011 ± 0 . 011)% for $$ {\Lambda}_c^{+} $$ Λ c + → Σ + K + π − , (0 . 414 ± 0 . 080 ± 0 . 030 ± 0 . 023)% for $$ {\Lambda}_c^{+} $$ Λ c + → Σ + ϕ and (0 . 197 ± 0 . 036 ± 0 . 009 ± 0 . 011)% for $$ {\Lambda}_c^{+} $$ Λ c + → Σ + K + K − (non- ϕ ). In all the above results, the first uncertainties are statistical, the second are systematic and the third are from external input of the branching fraction of $$ {\Lambda}_c^{+} $$ Λ c + → Σ + π + π − . Since no signal for $$ {\Lambda}_c^{+} $$ Λ c + → Σ + K + π − π 0 is observed, the upper limit of its branching fraction is determined to be 0.13% at the 90% confidence level.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2023
    detail.hit.zdb_id: 2027350-2
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  • 7
    In: The European Physical Journal C, Springer Science and Business Media LLC, Vol. 82, No. 11 ( 2022-11-09)
    Abstract: The decay $$D \rightarrow K^-\pi ^+$$ D → K - π + is studied in a sample of quantum-correlated $$D{\bar{D}}$$ D D ¯ pairs, based on a data set corresponding to an integrated luminosity of 2.93 fb $$^{-1}$$ - 1 collected at the $$\psi (3770)$$ ψ ( 3770 ) resonance by the BESIII experiment. The asymmetry between $$C\!P$$ C P -odd and $$C\!P$$ C P -even eigenstate decays into $$K^-\pi ^+$$ K - π + is determined to be $${{\mathcal {A}}}_{K\pi } = 0.132 \pm 0.011 \pm 0.007$$ A K π = 0.132 ± 0.011 ± 0.007 , where the first uncertainty is statistical and the second is systematic. This measurement is an update of an earlier study exploiting additional tagging modes, including several decay modes involving a $$K^0_L$$ K L 0 meson. The branching fractions of the $$K^0_L$$ K L 0 modes are determined as input to the analysis in a manner that is independent of any strong phase uncertainty. Using the predominantly $$C\!P$$ C P -even tag $$D\rightarrow \pi ^+\pi ^-\pi ^0$$ D → π + π - π 0 and the ensemble of $$C\!P$$ C P -odd eigenstate tags, the observable $${{\mathcal {A}}}_{K\pi }^{\pi \pi \pi ^0}$$ A K π π π π 0 is measured to be $$0.130 \pm 0.012 \pm 0.008$$ 0.130 ± 0.012 ± 0.008 . The two asymmetries are sensitive to $$r_D^{K\pi }\cos \delta _D^{K\pi }$$ r D K π cos δ D K π , where $$r_D^{K\pi }$$ r D K π and $$\delta _D^{K\pi }$$ δ D K π are the ratio of amplitudes and phase difference, respectively, between the doubly Cabibbo-suppressed and Cabibbo-favoured decays. In addition, events containing $$D \rightarrow K^-\pi ^+$$ D → K - π + tagged by $$D \rightarrow K^0_{S,L} \pi ^+\pi ^-$$ D → K S , L 0 π + π - are studied in bins of phase space of the three-body decays. This analysis has sensitivity to both $$r_D^{K\pi }\cos \delta _D^{K\pi }$$ r D K π cos δ D K π and $$r_D^{K\pi }\sin \delta _D^{K\pi }$$ r D K π sin δ D K π . A fit to $${{\mathcal {A}}}_{K\pi }$$ A K π , $${{\mathcal {A}}}_{K\pi }^{\pi \pi \pi ^0}$$ A K π π π π 0 and the phase-space distribution of the $$D \rightarrow K^0_{S,L} \pi ^+\pi ^-$$ D → K S , L 0 π + π - tags yields $$\delta _D^{K\pi }= \left( 187.6 {^{+8.9}_{-9.7}}{^{+5.4}_{-6.4}} \right) ^{\circ }$$ δ D K π = 187.6 - 9.7 + 8.9 - 6.4 + 5.4 ∘ , where external constraints are applied for $$r_D^{K\pi }$$ r D K π and other relevant parameters. This is the most precise measurement of $$\delta _D^{K\pi }$$ δ D K π in quantum-correlated $$D{\bar{D}}$$ D D ¯ decays.
    Type of Medium: Online Resource
    ISSN: 1434-6052
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2022
    detail.hit.zdb_id: 1397769-6
    detail.hit.zdb_id: 1459069-4
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  • 8
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2023, No. 3 ( 2023-03-17)
    Abstract: Using a sample of (10 . 09 ± 0 . 04) × 10 9 J/ψ decays collected with the BESIII detector, partial wave analyses of the decay $$ J/\psi \to \gamma {K}_S^0{K}_S^0{\pi}^0 $$ J / ψ → γ K S 0 K S 0 π 0 are performed within the $$ {K}_S^0{K}_S^0{\pi}^0 $$ K S 0 K S 0 π 0 invariant mass region below 1.6 GeV/ c 2 . The covariant tensor amplitude method is used in both mass independent and mass dependent approaches. Both analysis approaches exhibit dominant pseudoscalar and axial vector components, and show good consistency for the other individual components. Furthermore, the mass dependent analysis reveals that the $$ {K}_S^0{K}_S^0{\pi}^0 $$ K S 0 K S 0 π 0 invariant mass spectrum for the pseudoscalar component can be well described with two isoscalar resonant states using relativistic Breit-Wigner model, i.e., the η (1405) with a mass of $$ 1391.7\pm {0.7}_{-0.3}^{+11.3} $$ 1391.7 ± 0.7 − 0.3 + 11.3 MeV/ c 2 and a width of $$ 60.8\pm {1.2}_{-12.0}^{+5.5} $$ 60.8 ± 1.2 − 12.0 + 5.5 MeV, and the η (1475) with a mass of $$ 1507.6\pm {1.6}_{-32.2}^{+15.5} $$ 1507.6 ± 1.6 − 32.2 + 15.5 MeV/ c 2 and a width of $$ 115.8\pm {2.4}_{-10.9}^{+14.8} $$ 115.8 ± 2.4 − 10.9 + 14.8 MeV. The first and second uncertainties are statistical and systematic, respectively. Alternate models for the pseudoscalar component are also tested, but the description of the $$ {K}_S^0{K}_S^0{\pi}^0 $$ K S 0 K S 0 π 0 invariant mass spectrum deteriorates significantly.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2023
    detail.hit.zdb_id: 2027350-2
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  • 9
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2021, No. 5 ( 2021-05)
    Abstract: The decays D → K − π + π + π − and D → K − π + π 0 are studied in a sample of quantum-correlated $$ D\overline{D} $$ D D ¯ pairs produced through the process e + e − → ψ (3770) → $$ D\overline{D} $$ D D ¯ , exploiting a data set collected by the BESIII experiment that corresponds to an integrated luminosity of 2.93 fb − 1 . Here D indicates a quantum superposition of a D 0 and a $$ {\overline{D}}^0 $$ D ¯ 0 meson. By reconstructing one neutral charm meson in a signal decay, and the other in the same or a different final state, observables are measured that contain information on the coherence factors and average strong-phase differences of each of the signal modes. These parameters are critical inputs in the measurement of the angle γ of the Unitarity Triangle in B − → DK − decays at the LHCb and Belle II experiments. The coherence factors are determined to be R K 3 π = $$ {0.52}_{-0.10}^{+0.12} $$ 0.52 − 0.10 + 0.12 and $$ {R}_{K{\pi \pi}^0} $$ R K ππ 0 = 0 . 78 ± 0 . 04, with values for the average strong-phase differences that are $$ {\delta}_D^{K3\pi }=\left({167}_{-19}^{+31}\right){}^{\circ} $$ δ D K 3 π = 167 − 19 + 31 ° and $$ {\delta}_D^{K{\pi \pi}^0}=\left({196}_{-15}^{+14}\right){}^{\circ} $$ δ D K ππ 0 = 196 − 15 + 14 ° , where the uncertainties include both statistical and systematic contributions. The analysis is re-performed in four bins of the phase-space of the D → K − π + π + π − to yield results that will allow for a more sensitive measurement of γ with this mode, to which the BESIII inputs will contribute an uncertainty of around 6°.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2021
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  • 10
    In: Journal of High Energy Physics, Springer Science and Business Media LLC, Vol. 2020, No. 8 ( 2020-08)
    Abstract: We measure the branching fractions for seven $$ {D}_s^{+} $$ D s + two-body decays to pseudo-scalar mesons, by analyzing data collected at $$ \sqrt{s} $$ s = 4 . 178 ∼ 4 . 226 GeV with the BESIII detector at the BEPCII collider. The branching fractions are determined to be $$ {\displaystyle \begin{array}{c}\mathcal{B}\left({D}_s^{+}\to {K}^{+}\eta \hbox{'}\right)=\left(2.68\pm 0.17\pm 0.17\pm 0.08\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to \eta \hbox{'}{\pi}^{+}\right)=\left(37.8\pm 0.4\pm 2.1\pm 1.2\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}^{+}\eta \right)=\left(1.62\pm 0.10\pm 0.03\pm 0.05\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to \eta {\pi}^{+}\right)=\left(17.41\pm 0.18\pm 0.27\pm 0.54\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}^{+}{K}_S^0\right)=\left(15.02\pm 0.10\pm 0.27\pm 0.47\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}_S^0{\pi}^{+}\right)=\left(1.109\pm 0.034\pm 0.023\pm 0.035\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}^{+}{\pi}^0\right)=\left(0.748\pm 0.049\pm 0.018\pm 0.035\right)\times {10}^{-3},\end{array}} $$ B D s + → K + η ' = 2.68 ± 0.17 ± 0.17 ± 0.08 × 10 − 3 , B D s + → η ' π + = 37.8 ± 0.4 ± 2.1 ± 1.2 × 10 − 3 , B D s + → K + η = 1.62 ± 0.10 ± 0.03 ± 0.05 × 10 − 3 , B D s + → η π + = 17.41 ± 0.18 ± 0.27 ± 0.54 × 10 − 3 , B D s + → K + K S 0 = 15.02 ± 0.10 ± 0.27 ± 0.47 × 10 − 3 , B D s + → K S 0 π + = 1.109 ± 0.034 ± 0.023 ± 0.035 × 10 − 3 , B D s + → K + π 0 = 0.748 ± 0.049 ± 0.018 ± 0.035 × 10 − 3 , where the first uncertainties are statistical, the second are systematic, and the third are from external input branching fraction of the normalization mode $$ {D}_s^{+} $$ D s + → K + K − π + . Precision of our measurements is significantly improved compared with that of the current world average values.
    Type of Medium: Online Resource
    ISSN: 1029-8479
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2020
    detail.hit.zdb_id: 2027350-2
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