Recognition: unknown
Mini-review of charmonium weak decays at BESIII
Pith reviewed 2026-05-15 00:19 UTC · model grok-4.3
The pith
BESIII establishes the tightest upper limits to date on rare weak decays of J/ψ and ψ(2S) using its record datasets.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The BESIII collaboration has used its large samples of J/ψ and ψ(2S) to perform dedicated searches for weak charmonium decays and has set the most stringent upper limits available on branching fractions for a range of semi-leptonic, non-leptonic, and FCNC channels.
What carries the argument
The large accumulated data samples of over 10^10 J/ψ events and 2.7×10^9 ψ(2S) events, together with the dedicated reconstruction and background-suppression analyses that convert non-observation into quantitative upper limits on branching fractions.
If this is right
- The limits constrain possible new-physics contributions to flavor-changing neutral currents in the charm sector.
- They provide quantitative benchmarks for non-perturbative QCD calculations of charmonium weak-decay rates.
- Improved bounds on semi-leptonic modes help test lepton-flavor universality in the charm region.
- The results serve as reference points for planning future searches at higher-luminosity tau-charm facilities.
Where Pith is reading between the lines
- If the current limits persist, they will narrow the parameter space for models that predict enhanced charm FCNC rates at the TeV scale.
- Similar analysis strategies could be extended to rare decays of other heavy quarkonia once sufficient data become available.
- Cross-checks between BESIII results and indirect constraints from B-factory or LHCb measurements would test consistency across different production mechanisms.
Load-bearing premise
The published analyses have correctly estimated all backgrounds, efficiencies, and systematic uncertainties so that the quoted upper limits accurately reflect the true experimental sensitivity.
What would settle it
An independent re-analysis of the same datasets or a new higher-luminosity run that observes a signal in any of the listed channels at a branching fraction below the current BESIII upper limit would invalidate the claimed sensitivity.
Figures
read the original abstract
The weak decays of charmonium, involving $J/\psi$ and $\psi(2S)$ states, are instrumental in probing both non-perturbative QCD dynamics and flavor structure of the standard model (SM). The extremely rare nature of charmonium weak decays makes them highly sensitive to new physics beyond the SM, particularly in channels heavily suppressed in the SM, such as flavor-changing neutral current (FCNC) decays. This review highlights the critical role of the BESIII experiment, which leverages an unprecedented dataset of over $10^{10}$ $J/\psi$ events and $2.7\times10^{9}$ $\psi(2S)$ events to push the sensitivity of charmonium weak decay searches. We present the latest and most stringent upper limits established by BESIII on various semi-leptonic, non-leptonic, and FCNC charmonium weak decay channels.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This mini-review compiles and summarizes published BESIII experimental results on rare weak decays of the J/ψ and ψ(2S) charmonium states. It covers semi-leptonic, non-leptonic, and FCNC channels, emphasizing the large datasets (>10^10 J/ψ events and 2.7×10^9 ψ(2S) events) that enable the most stringent upper limits to date on these processes, which are sensitive to non-perturbative QCD and potential new physics.
Significance. As a concise compilation of existing BESIII limits rather than new data or derivations, the review offers a useful reference consolidating experimental progress in highly suppressed charmonium decays. It correctly positions the results as probes of SM flavor structure without introducing unsupported extrapolations.
minor comments (2)
- [Abstract] Abstract: the dataset sizes are stated without reference to the specific BESIII publications or run periods from which they derive; adding one-sentence citations here would improve traceability for readers.
- [Introduction] The review should explicitly note in the introduction or conclusion that all quoted limits are taken directly from the cited original analyses and have not been re-derived or combined here.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of our mini-review, which correctly identifies it as a concise compilation of the most stringent BESIII upper limits on rare charmonium weak decays. We appreciate the recognition of its utility as a reference for SM flavor probes and non-perturbative QCD studies. No major comments were raised in the report, so we will address any minor editorial points in the revised version.
Circularity Check
No significant circularity identified
full rationale
The paper is a mini-review that compiles and summarizes already-published BESIII experimental upper limits on rare charmonium weak decays. It contains no derivations, predictions, fitted parameters, or first-principles calculations. All quoted limits are presented as external results from prior BESIII analyses rather than being re-derived or extrapolated within this manuscript. No self-citation chains, ansatzes, or renamings function as load-bearing steps; the review's claims rest on the existence of those independent experimental publications.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
X. Q. Li, X. Liu, and Z. T. Wei. Charm physics: A field full with challenges and opportunities. Front. Phys. China, 4:49, 2009. doi:10.1007/s11467-009-0003-0
-
[2]
H. B. Li and S. H. Zhu. Mini-review of rare charmonium decays at BESIII. Chin. Phys. C , 36:932, 2012. doi: 10.1088/1674-1137/36/10/003
-
[3]
Y. Meng, J. L. Dang, C. Liu, et al. First lattice QCD calculation of J/ ψ semileptonic decay containing D and Ds particles. Phys. Rev. D , 110(7):074510, 2024. doi: 10.1103/PhysRevD.110.074510
-
[4]
M. A. Sanchis-Lozano. On the search for weak decays of heavy quarkonium in dedicated heavy quark factories. Z. Phys. C , 62:271, 1994. doi:10.1007/BF01560243
-
[5]
Y. M. Wang, H. Zou, Z. T. Wei, et al. The Transition form-factors for semi-leptonic weak decays of J/ψ in QCD sum rules. Eur. Phys. J. C , 54:107, 2008. doi: 10.1140/epjc/s10052-007-0498-x
-
[6]
Y. L. Shen and Y. M. Wang. J/ψ weak decays in the covariant light-front quark model. Phys. Rev. D , 78: 074012, 2008. doi:10.1103/PhysRevD.78.074012
-
[7]
Z. J. Sun, Z. Q. Zhang, Y. Y. Yang, et al. Semileptonic and nonleptonic weak decays of ψ(1S, 2S) and ηc(1S, 2S) to D(s) in the covariant light-front approach. Eur. Phys. J. C, 84(1):65, 2024. doi:10.1140/epjc/s10052-024-12404- 6
-
[8]
R. Dhir and R. C. Verma. Effects of Flavor Dependence on Weak Decays of J/ψ and Υ. Adv. High Energy Phys. , 2013:706543, 2013. doi:10.1155/2013/706543
-
[9]
M. A. Ivanov and C. T. Tran. Exclusive decays J/ψ→D(∗) (s) + in a covariant constituent quark model with infrared confinement. Phys. Rev. D , 92(7):074030, 2015. doi:10.1103/PhysRevD.92.074030
-
[10]
T. Wang, Y. Jiang, H. Yuan, et al. Weak decays of J/ψ and Υ(1S). J. Phys. G , 44(4):045004, 2017. doi: 10.1088/1361-6471/aa5f68
-
[11]
K. K. Sharma and R. C. Verma. Rare decays of Ψ and Υ. Int. J. Mod. Phys. A , 14:937, 1999. doi: 10.1142/S0217751X99000464
-
[12]
R. C. Verma, A. N. Kamal, and A. Czarnecki. Hadronic weak decays of Ψ. Phys. Lett. B , 252:690, 1990. doi: 10.1016/0370-2693(90)90507-3
-
[13]
Y. M. Wang, H. Zou, Z. T. Wei, et al. Weak decays of J/ψ: The Non-leptonic case. Eur. Phys. J. C , 55:607,
-
[14]
doi:10.1140/epjc/s10052-008-0619-1
-
[15]
J. Sun, Y. Yang, J. Huang, et al. Study of the ψ(1s, 2s) and ηc(1s, 2s) weak decays into dm. Adv. High Energy Phys., 2016:5071671, 2016. doi:10.1155/2016/5071671
-
[16]
Y. M. Wang, H. Zou, Z. T. Wei, et al. Fcnc- induced semileptonic decays of j/psi in the standard model. J. Phys. G , 36:105002, 2009. doi:10.1088/0954- 3899/36/10/105002
- [17]
-
[18]
A. Datta, P. J. O’Donnell, S. Pakvasa, et al. Flavor changing processes in quarkonium decays. Phys. Rev. D , 60:014011, 1999. doi:10.1103/PhysRevD.60.014011
-
[19]
M. Ablikim et al. Design and Construction of the BESIII Detector. Nucl. Instrum. Meth. A , 614:345–399, 2010. doi:10.1016/j.nima.2009.12.050. (BESIII Collaboration)
-
[20]
BEPCII Performance and Beam Dynamics Studies on Luminosity
Chenghui Yu et al. BEPCII Performance and Beam Dynamics Studies on Luminosity. In the proceedings of the 7th International Particle Accelerator Conference ,
-
[21]
doi:10.18429/JACoW-IPAC2016-TUYA01
-
[22]
Predictions for bottomonium from a relativistic screened potential model,
M. Ablikim et al. Number of J/ψ events at BESIII. Chin. Phys. C , 46(7):074001, 2022. doi:10.1088/1674- 1137/ac5c2e. (BESIII Collaboration)
-
[23]
M. H. Liao et al. Experimental dataset from BESIII detector at Beijing electron–positron collider. Nucl. Sci. Tech., 36(11):218, 2025. doi:10.1007/s41365-025-01789-y
-
[24]
M. Ablikim et al. Determination of the number of ψ(3686) events taken at BESIII. Chin. Phys. C , 48(9): 8 093001, 2024. doi:10.1088/1674-1137/ad595b. (BESIII Collaboration)
-
[25]
M. Ablikim et al. Search for the rare semi-leptonic decay J/ψ → D−e+νe + c.c.. JHEP, (06):157, 2021. doi: 10.1007/JHEP06(2021)157. (BESIII Collaboration)
-
[26]
D. Binosi and L. Theußl. JaxoDraw: A Graph- ical user interface for drawing Feynman diagrams. Comput. Phys. Commun. , 161:76–86, 2004. doi: 10.1016/j.cpc.2004.05.001
-
[27]
S. Navas et al. Review of particle physics. Phys. Rev. D , 110(3):030001, 2024. doi:10.1103/PhysRevD.110.030001. Particle Data Group
-
[28]
C. T. Hill. Topcolor assisted technicolor. Phys. Lett. B , 345:483, 1995. doi:10.1016/0370-2693(94)01660-5
-
[29]
C. S. Aulakh and R. N. Mohapatra. Neutrino as the supersymmetric partner of the majoron. Phys. Lett. B , 119:136, 1982. doi:10.1016/0370-2693(82)90262-3
-
[30]
S. L. Glashow and S. Weinberg. Natural conservation laws for neutral currents. Phys. Rev. D , 15:1958, 1977. doi:10.1103/PhysRevD.15.1958
-
[31]
M. Ablikim et al. Search for the semi-muonic charmonium decay J/ψ → D−µ+νµ + c.c.. JHEP, (01):126, 2024. doi:10.1007/JHEP01(2024)126. (BESIII Collaboration)
-
[32]
Search for the charmonium semi-leptonic weak decay $J/\psi\rightarrow D_s^-e^+\nu_e+c.c.$
M. Ablikim et al. Search for the charmonium semi- leptonic weak decay J/ψ → D− s e+νe + c.c., 2026. URL https://arxiv.org/abs/2510.25100. (BESIII Collaboration)
work page internal anchor Pith review Pith/arXiv arXiv 2026
-
[33]
M. Ablikim et al. Search for the weak decays J/ψ → D(∗) s eνe + c.c.. Phys. Rev. D , 90(11):112014, 2014. doi: 10.1103/PhysRevD.90.112014. (BESIII Collaboration)
-
[34]
M. Ablikim et al. Search for the charmonium weak decays J/ψ → D− s ρ+ + c.c. and J/ψ → D− s π+ + c.c.. JHEP, (12):077, 2025. doi:10.1007/JHEP12(2025)077. (BESIII Collaboration)
-
[35]
M. Ablikim et al. Search for J/ ψ weak decays containing a D meson. Phys. Rev. D , 110(3):032020, 2024. doi: 10.1103/PhysRevD.110.032020. (BESIII Collaboration)
-
[36]
M. Ablikim et al. Search for the charmonium weak decay J/ψ → ¯D0 ¯K ∗0+c.c., 11 2025. URL https://arxiv.org/ abs/2511.16083. (BESIII Collaboration)
-
[37]
M. Ablikim et al. Search for the FCNC charmonium decay J/ ψ→ D0 µ+ µ-+ cc. JHEP, (04):061, 2025. doi: 10.1007/JHEP04(2025)061. (BESIII Collaboration)
-
[38]
M. Ablikim et al. Search for the rare decays J/ψ → D0e+e− + c.c. and ψ(3686) → D0e+e− + c.c.. Phys. Rev. D , 96(11):111101, 2017. doi: 10.1103/PhysRevD.96.111101. (BESIII Collaboration)
-
[39]
M. Ablikim et al. Search for the rare decay J/ψ→γD0+c.c. at BESIII. Phys. Rev. D, 110(11):112012,
-
[40]
doi:10.1103/PhysRevD.110.112012. (BESIII Collaboration)
-
[41]
M. Ablikim et al. Search for the rare decay of ψ(3686) → Λ+ c pe+e− + c.c. at BESIII. Phys. Rev. D , 97(9):091102, 2018. doi:10.1103/PhysRevD.97.091102. (BESIII Collaboration)
-
[42]
M. Ablikim et al. Search for the weak decay ψ(3686) → Λ+ c ¯Σ− + c.c. Chin. Phys. C , 47(1):013002, 2023. doi: 10.1088/1674-1137/ac9895. (BESIII Collaboration)
-
[43]
H. W. Ke, Y. Z. Chen, and X. Q. Li. The decay rate of J/ψ to Λc + ¯Σ+ in SM and beyond. Chin. Phys. Lett. , 28:071301, 2011. doi:10.1088/0256-307X/28/7/071301
-
[44]
X. C. Ai et al. Conceptual design report of the Super Tau-Charm Facility: the accelerator. Nucl. Sci. Tech. , 36(12):242, 2025. doi:10.1007/s41365-025-01833-x
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