*Phys Rev Lett ; 127(17): 171801, 2021 Oct 22.*

##### RESUMO

Using a dataset of 6.32 fb^{-1} of e^{+}e^{-} annihilation data collected with the BESIII detector at center-of-mass energies between 4178 and 4226 MeV, we have measured the absolute branching fraction of the leptonic decay D_{s}^{+}âτ^{+}ν_{τ} via τ^{+}âe^{+}ν_{e}ν[over ¯]_{τ}, and find B_{D_{s}^{+}âτ^{+}ν_{τ}}=(5.27±0.10±0.12)×10^{-2}, where the first uncertainty is statistical and the second is systematic. The precision is improved by a factor of 2 compared to the previous best measurement. Combining with f_{D_{s}^{+}} from lattice quantum chromodynamics calculations or the |V_{cs}| from the CKMfitter group, we extract |V_{cs}|=0.978±0.009±0.012 and f_{D_{s}^{+}}=(251.1±2.4±3.0) MeV, respectively. Combining our result with the world averages of B_{D_{s}^{+}âτ^{+}ν_{τ}} and B_{D_{s}^{+}âµ^{+}ν_{µ}}, we obtain the ratio of the branching fractions B_{D_{s}^{+}âτ^{+}ν_{τ}}/B_{D_{s}^{+}âµ^{+}ν_{µ}}=9.72±0.37, which is consistent with the standard model prediction of lepton flavor universality.

*Phys Rev Lett ; 127(12): 121802, 2021 Sep 17.*

##### RESUMO

The absolute branching fraction of Λâpµ^{-}ν[over ¯]_{µ} is reported for the first time based on an e^{+}e^{-} annihilation sample of 10×10^{9} J/ψ events collected with the BESIII detector at sqrt[s]=3.097 GeV. The branching fraction is determined to be B(Λâpµ^{-}ν[over ¯]_{µ})=[1.48±0.21(stat)±0.08(syst)]×10^{-4}, which is improved by about 30% in precision over the previous indirect measurements. Combining this result with the world average of B(Λâpe^{-}ν[over ¯]_{e}), we obtain the ratio {[Γ(Λâpµ^{-}ν[over ¯]_{µ})]/[Γ(Λâpe^{-}ν[over ¯]_{e})]} to be 0.178±0.028, which agrees with the standard model prediction assuming lepton flavor universality. The asymmetry of the branching fractions of Λâpµ^{-}ν[over ¯]_{µ} and Λ[over ¯]âp[over ¯]µ^{+}ν_{µ} is also determined, and no evidence for CP violation is found.

*Phys Rev Lett ; 127(8): 082002, 2021 Aug 20.*

##### RESUMO

We report a measurement of the observed cross sections of e^{+}e^{-}âJ/ψX based on 3.21 fb^{-1} of data accumulated at energies from 3.645 to 3.891 GeV with the BESIII detector operated at the BEPCII collider. In analysis of the cross sections, we measured the decay branching fractions of B(ψ(3686)âJ/ψX)=(64.4±0.6±1.6)% and B(ψ(3770)âJ/ψX)=(0.5±0.2±0.1)% for the first time. The energy-dependent line shape of these cross sections cannot be well described by two Breit-Wigner (BW) amplitudes of the expected decays ψ(3686)âJ/ψX and ψ(3770)âJ/ψX. Instead, it can be better described with one more BW amplitude of the decay R(3760)âJ/ψX. Under this assumption, we extracted the R(3760) mass M_{R(3760)}=3766.2±3.8±0.4 MeV/c^{2} , total width Γ_{R(3760)}^{tot}=22.2±5.9±1.4 MeV, and product of leptonic width and decay branching fraction Γ_{R(3760)}^{ee}B[R(3760)âJ/ψX]=(79.4±85.5±11.7) eV. The significance of the R(3760) is 5.3σ. The first uncertainties of these measured quantities are from fits to the cross sections and second systematic.

*Phys Rev Lett ; 126(9): 092002, 2021 Mar 05.*

##### RESUMO

We present an analysis of the process ψ(3686)âΩ^{-}Ω[over ¯]^{+} (Ω^{-}âK^{-}Λ, Ω[over ¯]^{+}âK^{+}Λ[over ¯], Λâpπ^{-}, Λ[over ¯]âp[over ¯]π^{+}) based on a dataset of 448×10^{6} ψ(3686) decays collected with the BESIII detector at the BEPCII electron-positron collider. The helicity amplitudes for the process ψ(3686)âΩ^{-}Ω[over ¯]^{+} and the decay parameters of the subsequent decay Ω^{-}âK^{-}Λ (Ω[over ¯]^{+}âK^{+}Λ[over ¯]) are measured for the first time by a fit to the angular distribution of the complete decay chain, and the spin of the Ω^{-} is determined to be 3/2 for the first time since its discovery more than 50 years ago.

*Phys Rev Lett ; 126(10): 102001, 2021 Mar 12.*

##### RESUMO

We report a study of the processes of e^{+}e^{-}âK^{+}D_{s}^{-}D^{*0} and K^{+}D_{s}^{*-}D^{0} based on e^{+}e^{-} annihilation samples collected with the BESIII detector operating at BEPCII at five center-of-mass energies ranging from 4.628 to 4.698 GeV with a total integrated luminosity of 3.7 fb^{-1}. An excess of events over the known contributions of the conventional charmed mesons is observed near the D_{s}^{-}D^{*0} and D_{s}^{*-}D^{0} mass thresholds in the K^{+} recoil-mass spectrum for events collected at sqrt[s]=4.681 GeV. The structure matches a mass-dependent-width Breit-Wigner line shape, whose pole mass and width are determined as (3982.5_{-2.6}^{+1.8}±2.1) MeV/c^{2} and (12.8_{-4.4}^{+5.3}±3.0) MeV, respectively. The first uncertainties are statistical and the second are systematic. The significance of the resonance hypothesis is estimated to be 5.3 σ over the contributions only from the conventional charmed mesons. This is the first candidate for a charged hidden-charm tetraquark with strangeness, decaying into D_{s}^{-}D^{*0} and D_{s}^{*-}D^{0}. However, the properties of the excess need further exploration with more statistics.

*Phys Rev Lett ; 124(24): 241802, 2020 Jun 19.*

##### RESUMO

We report the most precise measurements to date of the strong-phase parameters between D^{0} and D[over ¯]^{0} decays to K_{S,L}^{0}π^{+}π^{-} using a sample of 2.93 fb^{-1} of e^{+}e^{-} annihilation data collected at a center-of-mass energy of 3.773 GeV with the BESIII detector at the BEPCII collider. Our results provide the key inputs for a binned model-independent determination of the Cabibbo-Kobayashi-Maskawa angle Î³/Ï_{3} with B decays. Using our results, the decay model sensitivity to the Î³/Ï_{3} measurement is expected to be between 0.7° and 1.2°, approximately a factor of three smaller than that achievable with previous measurements, based on the studies of the simulated data. The improved precision of this work ensures that measurements of Î³/Ï_{3} will not be limited by knowledge of strong phases for the next decade. Furthermore, our results provide critical input for other flavor-physics investigations, including charm mixing, other measurements of CP violation, and the measurement of strong-phase parameters for other D-decay modes.

*Phys Rev Lett ; 124(24): 241803, 2020 Jun 19.*

##### RESUMO

Using 2.93 fb^{-1} of 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 14 hadronic D^{0(+)} decays to exclusive final states with an Î·, e.g., D^{0}âK^{-}π^{+}Î·, K_{S}^{0}π^{0}Î·, K^{+}K^{-}Î·, K_{S}^{0}K_{S}^{0}Î·, K^{-}π^{+}π^{0}Î·, K_{S}^{0}π^{+}π^{-}Î·, K_{S}^{0}π^{0}π^{0}Î·, and π^{+}π^{-}π^{0}Î·; D^{+}âK_{S}^{0}π^{+}Î·, K_{S}^{0}K^{+}Î·, K^{-}π^{+}π^{+}Î·, K_{S}^{0}π^{+}π^{0}Î·, π^{+}π^{+}π^{-}Î·, and π^{+}π^{0}π^{0}Î·. Among these decays, the D^{0}âK^{-}π^{+}Î· and D^{+}âK_{S}^{0}π^{+}Î· decays have the largest branching fractions, which are B(D^{0}âK^{-}π^{+}Î·)=(1.853±0.025_{stat}±0.031_{syst})% and B(D^{+}âK_{S}^{0}π^{+}Î·)=(1.309±0.037_{stat}±0.031_{syst})%, respectively. The charge-parity asymmetries for the six decays with highest event yields are determined, and no statistically significant charge-parity violation is found.

*Phys Rev Lett ; 124(23): 231801, 2020 Jun 12.*

##### RESUMO

By analyzing a data sample corresponding to an integrated luminosity of 2.93 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^{+}âÎ·µ^{+}ν_{µ} decay to be B_{D^{+}âÎ·µ^{+}ν_{µ}}=(10.4±1.0_{stat}±0.5_{syst})×10^{-4}. Using the world averaged value of B_{D^{+}âÎ·e^{+}ν_{e}}, the ratio of the two branching fractions is determined to be B_{D^{+}âÎ·µ^{+}ν_{µ}}/B_{D^{+}âÎ·e^{+}ν_{e}}=0.91±0.13_{(stat+syst)}, which agrees with the theoretical expectation of lepton flavor universality within uncertainty. By studying the differential decay rates in five four-momentum transfer intervals, we obtain the product of the hadronic form factor f_{+}^{Î·}(0) and the câd Cabibbo-Kobayashi-Maskawa matrix element |V_{cd}| to be f_{+}^{Î·}(0)|V_{cd}|=0.087±0.008_{stat}±0.002_{syst}. Taking the input of |V_{cd}| from the global fit in the standard model, we determine f_{+}^{Î·}(0)=0.39±0.04_{stat}±0.01_{syst}. On the other hand, using the value of f_{+}^{Î·}(0) calculated in theory, we find |V_{cd}|=0.242±0.022_{stat}±0.006_{syst}±0.033_{theory}.

*Phys Rev Lett ; 124(11): 112001, 2020 Mar 20.*

##### RESUMO

A partial-wave analysis is performed for the process e^{+}e^{-}âK^{+}K^{-}π^{0}π^{0} at the center-of-mass energies ranging from 2.000 to 2.644 GeV. The data samples of e^{+}e^{-} collisions, collected by the BESIII detector at the BEPCII collider with a total integrated luminosity of 300 pb^{-1}, are analyzed. The total Born cross sections for the process e^{+}e^{-}âK^{+}K^{-}π^{0}π^{0}, as well as the Born cross sections for the subprocesses e^{+}e^{-}âÏπ^{0}π^{0}, K^{+}(1460)K^{-}, K_{1}^{+}(1400)K^{-}, K_{1}^{+}(1270)K^{-}, and K^{*+}(892)K^{*-}(892), are measured versus the center-of-mass energy. The corresponding results for e^{+}e^{-}âK^{+}K^{-}π^{0}π^{0} and Ïπ^{0}π^{0} are consistent with those of BABAR with better precision. By analyzing the cross sections for the four subprocesses, K^{+}(1460)K^{-}, K_{1}^{+}(1400)K^{-}, K_{1}^{+}(1270)K^{-}, and K^{*+}(892)K^{*-}(892), a structure with mass M=(2126.5±16.8±12.4) MeV/c^{2} and width Γ=(106.9±32.1±28.1) MeV is observed with an overall statistical significance of 6.3σ, although with very limited significance in the subprocesses e^{+}e^{-}âK_{1}^{+}(1270)K^{-} and K^{*+}(892)K^{*-}(892). The resonant parameters of the observed structure suggest it can be identified with the Ï(2170), thus the results provide valuable input to the internal nature of the Ï(2170).

*Phys Rev Lett ; 124(4): 042001, 2020 Jan 31.*

##### RESUMO

The process of e^{+}e^{-}âpp[over ¯] is studied at 22 center-of-mass energy points (sqrt[s]) from 2.00 to 3.08 GeV, exploiting 688.5 pb^{-1} of data collected with the BESIII detector operating at the BEPCII collider. The Born cross section (σ_{pp[over ¯]}) of e^{+}e^{-}âpp[over ¯] is measured with the energy-scan technique and it is found to be consistent with previously published data, but with much improved accuracy. In addition, the electromagnetic form-factor ratio (|G_{E}/G_{M}|) and the value of the effective (|G_{eff}|), electric (|G_{E}|), and magnetic (|G_{M}|) form factors are measured by studying the helicity angle of the proton at 16 center-of-mass energy points. |G_{E}/G_{M}| and |G_{M}| are determined with high accuracy, providing uncertainties comparable to data in the spacelike region, and |G_{E}| is measured for the first time. We reach unprecedented accuracy, and precision results in the timelike region provide information to improve our understanding of the proton inner structure and to test theoretical models which depend on nonperturbative quantum chromodynamics.

*Phys Rev Lett ; 123(23): 231801, 2019 Dec 06.*

##### RESUMO

By analyzing a 2.93 fb^{-1} data sample of e^{+}e^{-} collisions, recorded at a center-of-mass energy of 3.773 GeV with the BESIII detector operated at the BEPCII collider, we report the first observation of the semileptonic D^{+} transition into the axial-vector meson D^{+}âK[over ¯]_{1}(1270)^{0}e^{+}ν_{e} with a statistical significance greater than 10σ. Its decay branching fraction is determined to be B[D^{+}âK[over ¯]_{1}(1270)^{0}e^{+}ν_{e}]=(2.30±0.26_{-0.21}^{+0.18}±0.25)×10^{-3}, where the first and second uncertainties are statistical and systematic, respectively, and the third originates from the input branching fraction of K[over ¯]_{1}(1270)^{0}âK^{-}π^{+}π^{0}.

*Phys Rev Lett ; 123(12): 122003, 2019 Sep 20.*

##### RESUMO

The exclusive process e^{+}e^{-}âΛΛ[over ¯], with Λâpπ^{-} and Λ[over ¯]âp[over ¯]π^{+}, has been studied at sqrt[s]=2.396 GeV for measurement of the timelike Λ electric and magnetic form factors, G_{E} and G_{M}. A data sample, corresponding to an integrated luminosity of 66.9 pb^{-1}, was collected with the BESIII detector for this purpose. A multidimensional analysis with a complete decomposition of the spin structure of the reaction enables a determination of the modulus of the ratio R=|G_{E}/G_{M}| and, for the first time for any baryon, the relative phase ΔΦ=Φ_{E}-Φ_{M}. The resulting values are R=0.96±0.14(stat)±0.02(syst) and ΔΦ=37°±12°(stat)±6°(syst), respectively. These are obtained using the recently established and most precise value of the asymmetry parameter α_{Λ}=0.750±0.010 measured by BESIII. In addition, the cross section is measured with unprecedented precision to be σ=118.7±5.3(stat)±5.1(syst) pb, which corresponds to an effective form factor of |G|=0.123±0.003(stat)±0.003(syst). The contribution from two-photon exchange is found to be negligible. Our result enables the first complete determination of baryon timelike electromagnetic form factors.

*Phys Rev Lett ; 123(11): 112001, 2019 Sep 13.*

##### RESUMO

We present the first amplitude analysis of the decay D_{s}^{+}âπ^{+}π^{0}Î·. We use an e^{+}e^{-} collision data sample corresponding to an integrated luminosity of 3.19 fb^{-1} collected with the BESIII detector at a center-of-mass energy of 4.178 GeV. We observe for the first time the W-annihilation dominant decays D_{s}^{+}âa_{0}(980)^{+}π^{0} and D_{s}^{+}âa_{0}(980)^{0}π^{+}. We measure the absolute branching fraction B(D_{s}^{+}âa_{0}(980)^{+(0)}π^{0^{(}+)},a_{0}(980)^{+(0)}âπ^{+(0)}Î·)=(1.46±0.15_{stat}±0.23_{sys})%, which is larger than the branching fractions of other measured pure W-annihilation decays by at least one order of magnitude. In addition, we measure the branching fraction of D_{s}^{+}âπ^{+}π^{0}Î· with significantly improved precision.

*Phys Rev Lett ; 122(20): 202001, 2019 May 24.*

##### RESUMO

Using a total of 9.0 fb^{-1} of e^{+}e^{-} collision data with center-of-mass energies between 4.15 and 4.30 GeV collected by the BESIII detector, we search for the processes e^{+}e^{-}âÎ³X(3872) with X(3872)âπ^{0}χ_{cJ} for J=0, 1, 2. We report the first observation of X(3872)âπ^{0}χ_{c1}, a new decay mode of the X(3872), with a statistical significance of more than 5σ for all systematic fit variations. Normalizing to the previously established process e^{+}e^{-}âÎ³X(3872) with X(3872)âπ^{+}π^{-}J/ψ, we find B(X(3872)âπ^{0}χ_{c1})/B(X(3872)âπ^{+}π^{-}J/ψ)=0.88_{-0.27}^{+0.33}±0.10, where the first error is statistical and the second is systematic. We set 90% confidence level upper limits on the corresponding ratios for the decays to π^{0}χ_{c0} and π^{0}χ_{c2} of 19 and 1.1, respectively.

*Phys Rev Lett ; 122(14): 142002, 2019 Apr 12.*

##### RESUMO

Based on a sample of (1310.6±7.0)×10^{6}J/ψ events collected with the BESIII detector, we present measurements of J/ψ and Î·^{'} absolute branching fractions using the process J/ψâÎ³Î·^{'}. By analyzing events where the radiative photon converts into an e^{+}e^{-} pair, the branching fraction for J/ψâÎ³Î·^{'} is measured to be (5.27±0.03±0.05)×10^{-3}. The absolute branching fractions of the five dominant decay channels of the Î·^{'} are then measured for the first time and are determined to be B(Î·^{'}âÎ³π^{+}π^{-})=(29.90±0.03±0.55)%, B(Î·^{'}âÎ·π^{+}π^{-})=(41.24±0.08±1.24)%, B(Î·^{'}âÎ·π^{0}π^{0})=(21.36±0.10±0.92)%, B(Î·^{'}âÎ³ω)=(2.489±0.018±0.074)%, and B(Î·^{'}âÎ³Î³)=(2.331±0.012±0.035)%, where the first uncertainties are statistical and the second systematic.

*Phys Rev Lett ; 122(12): 121801, 2019 Mar 29.*

##### RESUMO

Using e^{+}e^{-} annihilation data corresponding to an integrated luminosity of 3.19 fb^{-1} collected at a center-of-mass energy of 4.178 GeV with the BESIII detector, we measure the absolute branching fractions B_{D_{s}^{+}âÎ·e^{+}ν_{e}}=(2.323±0.063_{stat}±0.063_{syst})% and B_{D_{s}^{+}âÎ·^{'}e^{+}ν_{e}}=(0.824±0.073_{stat}±0.027_{syst})% via a tagged analysis technique, where one D_{s} is fully reconstructed in a hadronic mode. Combining these measurements with previous BESIII measurements of B_{D^{+}âÎ·^{(')}e^{+}ν_{e}}, the Î·-Î·^{'} mixing angle in the quark flavor basis is determined to be Ï_{P}=(40.1±2.1_{stat}±0.7_{syst})°. From the first measurements of the dynamics of D_{s}^{+}âÎ·^{(')}e^{+}ν_{e} decays, the products of the hadronic form factors f_{+}^{Î·^{(')}}(0) and the Cabibbo-Kobayashi-Maskawa matrix element |V_{cs}| are determined with different form factor parametrizations. For the two-parameter series expansion, the results are f_{+}^{Î·}(0)|V_{cs}|=0.4455±0.0053_{stat}±0.0044_{syst} and f_{+}^{Î·^{'}}(0)|V_{cs}|=0.477±0.049_{stat}±0.011_{syst}.

*Phys Rev Lett ; 122(10): 102002, 2019 Mar 15.*

##### RESUMO

The cross section of the process e^{+}e^{-}âπ^{+}D^{0}D^{*-} for center-of-mass energies from 4.05 to 4.60 GeV is measured precisely using data samples collected with the BESIII detector operating at the BEPCII storage ring. Two enhancements are clearly visible in the cross section around 4.23 and 4.40 GeV. Using several models to describe the dressed cross section yields stable parameters for the first enhancement, which has a mass of 4228.6±4.1±6.3 MeV/c^{2} and a width of 77.0±6.8±6.3 MeV, where the first uncertainties are statistical and the second ones are systematic. Our resonant mass is consistent with previous observations of the Y(4220) state and the theoretical prediction of a DD[over ¯]_{1}(2420) molecule. This result is the first observation of Y(4220) associated with an open-charm final state. Fits with three resonance functions with additional Y(4260), Y(4320), Y(4360), ψ(4415), or a new resonance do not show significant contributions from either of these resonances. The second enhancement is not from a single known resonance. It could contain contributions from ψ(4415) and other resonances, and a detailed amplitude analysis is required to better understand this enhancement.

*Phys Rev Lett ; 122(1): 011804, 2019 Jan 11.*

##### RESUMO

Using e^{+}e^{-} annihilation data of 2.93 fb^{-1} collected at center-of-mass energy sqrt[s]=3.773 GeV with the BESIII detector, we measure the absolute branching fraction of D^{0}âK^{-}µ^{+}ν_{µ} with significantly improved precision: B_{D^{0}âK^{-}µ^{+}ν_{µ}}=(3.413±0.019_{stat}±0.035_{syst})%. Combining with our previous measurement of B_{D^{0}âK^{-}e^{+}ν_{e}}, the ratio of the two branching fractions is determined to be B_{D^{0}âK^{-}µ^{+}ν_{µ}}/B_{D^{0}âK^{-}e^{+}ν_{e}}=0.974±0.007_{stat}±0.012_{syst}, which agrees with the theoretical expectation of lepton flavor universality within the uncertainty. A study of the ratio of the two branching fractions in different four-momentum transfer regions is also performed, and no evidence for lepton flavor universality violation is found with current statistics. Taking inputs from global fit in the standard model and lattice quantum chromodynamics separately, we determine f_{+}^{K}(0)=0.7327±0.0039_{stat}±0.0030_{syst} and |V_{cs}|=0.955±0.005_{stat}±0.004_{syst}±0.024_{LQCD}.

*Phys Rev Lett ; 122(6): 062001, 2019 Feb 15.*

##### RESUMO

Using a data sample corresponding to an integrated luminosity of 2.93 fb^{-1} recorded by the BESIII detector at a center-of-mass energy of 3.773 GeV, we present an analysis of the decays D^{0}âπ^{-}π^{0}e^{+}ν_{e} and D^{+}âπ^{-}π^{+}e^{+}ν_{e}. By performing a partial wave analysis, the π^{+}π^{-} S-wave contribution to D^{+}âπ^{-}π^{+}e^{+}ν_{e} is observed to be (25.7±1.6±1.1)% with a statistical significance greater than 10σ, besides the dominant P-wave contribution. This is the first observation of the S-wave contribution. We measure the branching fractions B(D^{0}âρ^{-}e^{+}ν_{e})=(1.445±0.058±0.039)×10^{-3}, B(D^{+}âρ^{0}e^{+}ν_{e})=(1.860±0.070±0.061)×10^{-3}, and B(D^{+}âf_{0}(500)e^{+}ν_{e},f_{0}(500)âπ^{+}π^{-})=(6.30±0.43±0.32)×10^{-4}. An upper limit of B(D^{+}âf_{0}(980)e^{+}ν_{e},f_{0}(980)âπ^{+}π^{-})<2.8×10^{-5} is set at the 90% confidence level. We also obtain the hadronic form factor ratios of Dâρe^{+}ν_{e} at q^{2}=0 assuming the single-pole dominance parametrization: r_{V}={[V(0)]/[A_{1}(0)]}=1.695±0.083±0.051, r_{2}={[A_{2}(0)]/[A_{1}(0)]}=0.845±0.056±0.039.

*Phys Rev Lett ; 122(6): 061801, 2019 Feb 15.*

##### RESUMO

We report on new measurements of Cabibbo-suppressed semileptonic D_{s}^{+} decays using 3.19 fb^{-1} of e^{+}e^{-} annihilation data sample collected at a center-of-mass energy of 4.178 GeV with the BESIII detector at the BEPCII collider. Our results include branching fractions B(D_{s}^{+}âK^{0}e^{+}ν_{e})=[3.25±0.38(stat)±0.16(syst)]×10^{-3} and B(D_{s}^{+}âK^{*0}e^{+}ν_{e})=[2.37±0.26(stat)±0.20(syst)]×10^{-3}, which are much improved relative to previous measurements, and the first measurements of the hadronic form-factor parameters for these decays. For D_{s}^{+}âK^{0}e^{+}ν_{e}, we obtain f_{+}(0)=0.720±0.084(stat)±0.013(syst), and for D_{s}^{+}âK^{*0}e^{+}ν_{e}, we find form-factor ratios r_{V}=V(0)/A_{1}(0)=1.67±0.34(stat)±0.16(syst) and r_{2}=A_{2}(0)/A_{1}(0)=0.77±0.28(stat)±0.07(syst).