Number of J/ψ events at BESIII Adlarson, P.; Ahmed, S.; Amoroso, A. ...
Chinese physics C,
07/2022, Letnik:
46, Številka:
7
Journal Article
Recenzirano
Odprti dostop
Abstract
Using inclusive decays of
, a precise determination of the number of
events collected with the BESIII detector was performed. For the two data sets taken in 2009 and 2012, the numbers of
...events were recalculated to be
and
, respectively; these numbers are in good agreement with the previous measurements. For the
sample taken in 2017–2019, the number of events was determined to be
. The total number of
events collected with the BESIII detector was determined to be
, where the uncertainty is dominated by systematic effects, and the statistical uncertainty is negligible.
We report the first measurements of absolute branching fractions for the W-exchange-only processes Λc+→Ξ0K+ and Λc+→Ξ(1530)0K+ with the double-tag technique, by analyzing an e+e− collision data ...sample, that corresponds to an integrated luminosity of 567 pb−1 collected at a center-of-mass energy of 4.6 GeV by the BESIII detector. The branching fractions are measured to be B(Λc+→Ξ0K+)=(5.90±0.86±0.39)×10−3 and B(Λc+→Ξ(1530)0K+)=(5.02±0.99±0.31)×10−3, where the first uncertainties are statistical and the second systematic. Our results are more precise than the previous relative measurements.
Abstract
From December 2019 to June 2021, the BESIII experiment collected approximately 5.85 fb
−1
of data at center-of-mass energies between 4.61 and 4.95 GeV. This is the highest collision energy ...BEPCII has reached to date. The accumulated
annihilation data samples are useful for studying charmonium(-like) states and charmed-hadron decays. By adopting a novel method of analyzing the production of
pairs in
annihilation, the center-of-mass energies are measured with a precision of
0.6 MeV. Integrated luminosities are measured with a precision of better than 1% by analyzing the events of large-angle Bhabha scattering. These measurements provide important inputs to analyses based on these data samples.
Based on 10 billion J/psi events collected at the BESIII experiment, a search for CP violation in Lambda decay is performed in the difference between CP-odd decay parameters alpha_ for Lambda -> p ...pi(-) and alpha(+) for (Lambda) over bar -> (p) over bar pi(+) by using the process e(+)e(-) -> J/psi -> Lambda(Lambda) over bar. With a five-dimensional fit to the full angular distributions of the daughter baryon, the most precise values for the decay parameters arc determined to be a_ = 0.7519 +/- 0.0036 +/- 0.0024 and alpha(+) = -0.7559 +/- 0.0036 +/- 0.0030, respectively. The Lambda and (Lambda) over bar averaged value of the decay parameter is extracted to be a(avg) = 0.7542 +/- 0.0010 +/- 0.0024 with unprecedented accuracy. The CP asymmetry A(CP) = (alpha_ + alpha(+))/(a_-alpha(+)) is determined to be -0.0025 +/- 0.0046 +/- 0.0012, which is one of the most precise measurements in the baryon sector. The reported results for the decay parameter will play an important role in the studies of the polarizations and CP violations for the strange, charmed and beauty baryons.
Recent results on
e
+
e
−
annihilation to hadrons from SND experiment at VEPP-2000 collider are presented. Corresponding data set is about 200 pb
−1
of integrated luminosity collected at the energy ...region below 2 GeV. The processes
e
+
e
−
→ π
+
π
−
, π
0
γ, ωπ
0
, π
+
π
−
π
0
, ηπ
+
π
−
π
0
,
η
, π
+
π
−
4π
0
have been studied. Searches for
e
+
e
−
annihilation to
C
-even resonances η and
f
1(1285) were done.
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 D0 → π−π0e+νe ...and D+ → π−π+e+νe. By performing a partial wave analysis, the π+π− S-wave contribution to D+ → π−π+e+νe 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(D0 → ρ−e+νe) = (1.445 ± 0.058 ± 0.039) × 10−3, B(D+ → ρ0e+νe) = (1.860 ± 0.070 ± 0.061) × 10−3, and B(D+ → f0(500)e+νe, f0(500) → π+π−) = (6.30 ± 0.43 ± 0.32) × 10−4. An upper limit of B(D+ → f0(980)e+νe, f0(980) → π+π−) < 2.8 × 10−5 is set at the 90% confidence level. We also obtain the hadronic form factor ratios of D → ρe+νe at q2 = 0 assuming the single-pole dominance parametrization: rV = {V(0)/A1(0)} = 1.695 ± 0.083 ± 0.051, r2 = {A2(0)/A1(0)} = 0.845 ± 0.056 ± 0.039.
Using a data set of 2.93 fb taken at a center-of-mass energy root s = 3.773 GeV with the BESIII detector at the BEPCII collider, we perform a search for an extra U(1) gauge boson, also denoted as a ...dark photon. We examine the initial state radiation reactions e(+)e(-) -> e(+)e(-) gamma(ISR) and e(+)e(-) -> mu(+)mu(-) gamma(ISR) for this search, where the dark photon would appear as an enhancement in the invariant mass distribution of the leptonic pairs. We observe no obvious enhancement in the mass range between 1.5 and 3.4 GeV/c(2) and set a 90% confidence level upper limit on the mixing strength of the dark photon and the Standard Model photon. We obtain a competitive limit in the tested mass range.
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 BDs+→ηe+νe = (2.323±0.063stat ± 0.063syst)% and BDs+→η′e+νe = (0.824±0.073stat ± 0.027syst)% via a tagged analysis technique, where one Ds is fully reconstructed in a hadronic mode. Combining these measurements with previous BESIII measurements of BD+→η(′)e+νe, the η−η′ mixing angle in the quark flavor basis is determined to be ϕP = (40.1±2.1stat ± 0.7syst)°. From the first measurements of the dynamics of Ds+ → η(′)e+νe decays, the products of the hadronic form factors f+η(′)(0) and the Cabibbo-Kobayashi-Maskawa matrix element |Vcs| are determined with different form factor parametrizations. For the two-parameter series expansion, the results are f+η(0)|Vcs| = 0.4455±0.0053stat±0.0044syst and f+η′(0)|Vcs|=0.477±0.049stat±0.011syst.
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