Weiping Wang

Dr. Weiping Wang

orcid

Research Focus & Metrics

Academic Career Length

6Years (2021-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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10 September 2025 in Physics Reports
Verified
Journal Article
Open access
RAR. Aliberti
R. Aliberti
TAT. Aoyama
T. Aoyama
EBE. Balzani
E. Balzani
ABA. Bashir
A. Bashir
GBG. Benton
G. Benton
AZA.S. Zhevlakov
A.S. Zhevlakov

10 February 2022 in Physical Review Letters
Verified
Journal Article
Open access
PDF file
MAM Ablikim
M Ablikim
MAM N Achasov
M N Achasov
PAP Adlarson
P Adlarson
SAS Ahmed
S Ahmed
MAM Albrecht
M Albrecht
BCBESIII Collaboration
BESIII Collaboration
Based on electron-positron collision data collected with the BESIII detector operating at the Beijing Electron-Positron Collider II storage rings, the value of R≡σ(e+e−→hadrons)/σ(e+e−→μ+μ−) is measured at 14 center-of-mass energies from 2.2324 to 3.6710 GeV. The resulting uncertainties are less than 3.0% and are dominated by systematic uncertainties.

18 May 2026 in Physical Review Letters
Verified
Journal Article
Open access
MAM. Ablikim
M. Ablikim
MAM. N. Achasov
M. N. Achasov
PAP. Adlarson
P. Adlarson
XAX. C. Ai
X. C. Ai
RAR. Aliberti
R. Aliberti
JZJ. H. Zou
J. H. Zou
A search for C P violation with an entangled system of Ξ − Ξ ¯ + pairs is performed, using ( 10 , 087 ± 44 ) × 10 6 J / ψ events collected with the BESIII experiment. A nine-dimensional helicity amplitude is used to fit e + e − → J / ψ → Ξ − Ξ ¯ + and its subsequent decays. The Ξ − and Ξ ¯ + decay parameters are determined with higher precision compared to the best results reported so far. Furthermore, the strong phase difference, ( δ P − δ S ) = ( 0.3 ± 1.2 ± 0.2 ) × 10 − 2 rad , and the weak phase difference, ( ξ P − ξ S ) = ( − 0.2 ± 1.2 ± 0.1 ) × 10 − 2 rad , are directly determined. These are the most precise measurements to date. The C P asymmetry observables A C P Ξ = ( − 7.8 ± 4.8 ± 0.8 ) × 10 − 3 and Δ ϕ C P Ξ = ( 0.6 ± 5.1 ± 0.2 ) × 10 − 3 rad are determined, which are consistent with C P conservation. In addition, independent measurements of the Λ decay parameter and C P asymmetry A C P Λ = ( − 2.9 ± 4.3 ± 0.7 ) × 10 − 3 are also obtained, which are in agreement with the previous measurements, but with much improved precision.

21 December 2021 in Symmetry
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Journal Article
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WWWeiping Wang
Weiping Wang
XZXiaorong Zhou
Xiaorong Zhou
RFRinaldo Baldini Ferroli
Rinaldo Baldini Ferroli
GHGuangshun Huang
Guangshun Huang
As the lightest charmed baryon, precision measurement of the pair production cross section of Λc+ provides unprecedented experimental information for the investigation of baryon production mechanism. In addition, the extraction of the polar angle distributions of the outgoing Λc+ in the annihilation of the electron–positron help to determine its electromagnetic form factors, which is currently the unique key to access the internal structure of the baryons. In this article, the measurement of e+e−→Λc+Λ¯c− process via the initial state radiation technique at Belle detector and direct electron–positron annihilation at BESIII with discrete center-of-mass energies near threshold are briefly reviewed. In addition, the electromagnetic form factor ratios of Λc+ measured by BESIII are also investigated. A few theoretical models that parameterize the center-of-mass energy dependence of the cross section and electromagnetic form factors of baryon are introduced and the contributions of Λc+ data to them are discussed.

19 November 2025 in Journal of High Energy Physics
Verified
Journal Article
Open access
PDF file
MAM Ablikim
M Ablikim
MAM Achasov
M Achasov
PAP Adlarson
P Adlarson
XAX Ai
X Ai
RAR Aliberti
R Aliberti
JZJ Zu
J Zu
A bstract: Using e + e − collision data corresponding to a total integrated luminosity of 20 fb − 1 collected with the BESIII detector at the BEPCII collider, we present a measurement of the Born cross section for the process $$ {e}^{+}{e}^{-}\to p{K}^{-}{K}^{-}{\overline{\Xi}}^{+} $$ e + e − → p K − K − Ξ ¯ + at 39 center-of-mass energies between 3.5 and 4.9 GeV with a partial reconstruction technique. By performing a fit to the dressed cross section of $$ {e}^{+}{e}^{-}\to p{K}^{-}{K}^{-}{\overline{\Xi}}^{+} $$ e + e − → p K − K − Ξ ¯ + with a power law function for continuum production and one resonance at a time for the ψ (3770), ψ (4040), ψ (4160), ψ (4230), ψ (4360), ψ (4415) or ψ (4660), respectively, the upper limits for the product of partial electronic width and branching fraction into the final state $$ p{K}^{-}{K}^{-}{\overline{\Xi}}^{+} $$ p K − K − Ξ ¯ + for these resonances are determined at the 90% confidence level.

17 February 2026 in Physical Review D
Verified
Journal Article
Open access
MAM. Ablikim
M. Ablikim
MAM. N. Achasov
M. N. Achasov
PAP. Adlarson
P. Adlarson
XAX. C. Ai
X. C. Ai
RAR. Aliberti
R. Aliberti
JZJ. Zu
J. Zu
We report a direct search for a new gauge boson, X , with a mass of 17 MeV / c 2 , which could explain the anomalous excess of e + e − pairs observed in the Be 8 nuclear transitions. The search is conducted in the charmonium decays χ c J → X J / ψ ( J = 0 , 1 , 2 ) via the radiative transition ψ ( 3686 ) → γ χ c J using ( 2712.4 ± 14.3 ) × 10 6 ψ ( 3686 ) events collected with the BESIII detector at the BEPCII collider. No significant signal is observed, and the updated upper limit on the coupling strength of charm quark and the new gauge boson, ε c , is set to be | ε c | < 1.2 × 10 − 2 at 90% confidence level. We also report new constraints on the mixing strength ε between the Standard Model photon and dark photon γ ′ in the mass range from 5 to 300 MeV / c 2 . The upper limits at 90% confidence level vary within ( 2.5 – 17.5 ) × 10 − 3 depending on the γ ′ mass.