Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Potential of the reaction e+e−→pp¯π0 for constructing higher ρ-meson spectroscopy above 2.4 GeV

Dan Guo

Jun-Zhang Wang*

Qin-Song Zhou†

  • School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, People’s Republic of China

  • Department of Physics, Chongqing University, Chongqing 401331, People’s Republic of China and School of Physics and Center of High Energy Physics, Peking University, Beijing 100871, People’s Republic of China

  • School of Physical Science and Technology, Inner Mongolia University, Hohhot 010021, People’s Republic of China; Research Center for Quantum Physics and Technologies, Inner Mongolia University, Hohhot 010021, People’s Republic of China and Inner Mongolia Key Laboratory of Microscale Physics and Atomic Manufacturing, Hohhot 010021, People’s Republic of China

  • *Contact author: wangjzh@cqu.edu.cn
  • †Contact author: zhouqs@imu.edu.cn

Phys. Rev. D 112, 114029 – Published 18 December, 2025

DOI: https://doi.org/10.1103/w5gh-lq88

Abstract

The spectrum of light unflavored vector mesons above 2.4 GeV has not yet been firmly established experimentally. In this work, we demonstrate that the process e+e−→pp¯π serves as a particularly promising channel as a probe for higher isovector ρ excitations. In contrast to typical electron-positron annihilation processes into purely light-meson final states, the reaction e+e−→pp¯π benefits from a relatively low continuum background, on the order of (50∼100)  pb around 2.4 GeV, which enhances the visibility of even modest resonance contributions. In addition, the comparatively high production threshold further suppresses potential contamination from lower ρ-meson excitations. Our analysis based on effective Lagrangian approach indicates that the observed line shape of the e+e−→pp¯π cross section measured by the Beijing Spectrometer (BESIII) Experiment can be naturally interpreted by including the ρ(5S) and ρ(6S) contributions, namely the fourth and fifth radial excitations of ρ(770). In particular, the pronounced rise of the cross section near 2.4 GeV provides strong evidence for the contribution of ρ(5S) signal. Their branching ratios to the pp¯π final state are found to be below 4%, which do not contradict with usual expectations. In addition, we evaluate pion-induced production of these two ρ-meson states as a complementary probe, offering useful guidance for the relevant experiments such as the Common Muon and Proton Apparatus for Structure and Spectroscopy.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (48)

  1. E. Klempt and A. Zaitsev, Glueballs, Hybrids, multiquarks. experimental facts versus QCD inspired concepts, Phys. Rep. 454, 1 (2007).
  2. W. Ochs, The status of glueballs, J. Phys. G 40, 043001 (2013).
  3. A. J. Bevan et al. (BABAR Collaboration and Belle Collaboration), The physics of the B factories, Eur. Phys. J. C 74, 3026 (2014).
  4. E. Kou et al. (Belle-II Collaboration), The Belle II physics book, Prog. Theor. Exp. Phys. 2019, 123C01 (2019); 2020, 029201(E) (2020).
  5. D. M. Asner, T. Barnes, J. M. Bian, I. I. Bigi, N. Brambilla, I. R. Boyko, V. Bytev, K. T. Chao, J. Charles and H. X. Chen et al., Physics at BES-III, Int. J. Mod. Phys. A 24, S1-794 (2009); arXiv:0809.1869.
  6. M. Ablikim et al. (BESIII Collaboration), Future physics programme of BESIII, Chin. Phys. C 44, 040001 (2020).
  7. S. Godfrey and J. Napolitano, Light meson spectroscopy, Rev. Mod. Phys. 71, 1411 (1999).
  8. S. S. Fang (BESIII Collaboration), Light hadron physics at BES experiment, Symposium on 30 Years of BES Physic (2020), pp. 116–122.
  9. G. S. Huang, R measurements and QCD studies at the BES experiments, Symposium on 30 Years of BES Physic (2020), pp. 145–151.
  10. S. Navas et al. (Particle Data Group), Review of particle physics, Phys. Rev. D 110, 030001 (2024).
  11. B. Aubert et al. (BABAR Collaboration), Structure at 2175-MeV in e+e−→ϕf0(980) observed via initial-state radiation, Phys. Rev. D 74, 091103 (2006).
  12. B. Aubert et al. (BABAR Collaboration), Observation of a broad structure in the π+π−J/ψ mass spectrum around 4.26  GeV/c2, Phys. Rev. Lett. 95, 142001 (2005).
  13. S. L. Zhu, The possible interpretations of Y(4260), Phys. Lett. B 625, 212 (2005).
  14. T. Barnes, N. Black, and P. R. Page, Strong decays of strange quarkonia, Phys. Rev. D 68, 054014 (2003).
  15. C. Q. Pang, Excited states of ϕ meson, Phys. Rev. D 99, 074015 (2019).
  16. X. Wang, Z. F. Sun, D. Y. Chen, X. Liu, and T. Matsuki, Non-strange partner of strangeonium-like state Y(2175), Phys. Rev. D 85, 074024 (2012).
  17. G. J. Ding and M. L. Yan, Y(2175): Distinguish hybrid state from higher quarkonium, Phys. Lett. B 657, 49 (2007).
  18. J. Z. Wang, L. M. Wang, X. Liu, and T. Matsuki, Deciphering the light vector meson contribution to the cross sections of e+e− annihilations into the open-strange channels through a combined analysis, Phys. Rev. D 104, 054045 (2021).
  19. M. Ablikim et al. (BESIII Collaboration), Observation of a resonant structure in e+e−→ωη and another in e+e−→ωπ0 at center-of-mass energies between 2.00 and 3.08 GeV, Phys. Lett. B 813, 136059 (2021).
  20. M. Ablikim et al. (BESIII Collaboration), Measurement of the e+e−→ωπ0π0 cross section at center-of-mass energies from 2.0 to 3.08 GeV, Phys. Rev. D 105, 032005 (2022).
  21. Q. S. Zhou, J. Z. Wang, and X. Liu, Role of the ω(4S) and ω(3D) states in mediating the e+e−→ωη and ωπ0π0 processes, Phys. Rev. D 106, 034010 (2022).
  22. Z. Y. Bai, Q. S. Zhou, and X. Liu, Role of 4S−3D mixing in explaining the ω-like Y(2119) observed in e+e−→ρπ and ρ(1450)π, Phys. Rev. D 111, 054013 (2025).
  23. M. Ablikim et al. (BESIII Collaboration), Study of e+e−→π+π−π0 at s from 2.00 to 3.08 GeV at BESIII, Phys. Rev. D 110, 032005 (2024).
  24. S. Godfrey and N. Isgur, Mesons in a relativized quark model with chromodynamics, Phys. Rev. D 32, 189 (1985).
  25. T. Barnes, F. E. Close, P. R. Page, and E. S. Swanson, Higher quarkonia, Phys. Rev. D 55, 4157 (1997).
  26. D. Ebert, R. N. Faustov, and V. O. Galkin, Mass spectra and Regge trajectories of light mesons in the relativistic quark model, Phys. Rev. D 79, 114029 (2009).
  27. Z. Y. Li, D. M. Li, E. Wang, W. C. Yan, and Q. T. Song, Assignments of the Y(2040), ρ(1900), and ρ(2150) in the quark model, Phys. Rev. D 104, 034013 (2021).
  28. L. P. He, X. Wang, and X. Liu, Towards two-body strong decay behavior of higher ρ and ρ3 mesons, Phys. Rev. D 88, 034008 (2013).
  29. J. C. Feng, X. W. Kang, Q. F. Lü, and F. S. Zhang, Possible assignment of excited light S31 vector mesons, Phys. Rev. D 104, 054027 (2021).
  30. T. Hilger, M. Gomez-Rocha, and A. Krassnigg, Light-quarkonium spectra and orbital-angular-momentum decomposition in a Bethe–Salpeter-equation approach, Eur. Phys. J. C 77, 625 (2017).
  31. T. Branz, T. Gutsche, V. E. Lyubovitskij, I. Schmidt, and A. Vega, Light and heavy mesons in a soft-wall holographic approach, Phys. Rev. D 82, 074022 (2010).
  32. G. L. Yu, Z. G. Wang, X. W. Wang, and H. J. Wang, The ground states and the first radially excited states of D-wave vector ρ and ϕ mesons, Int. J. Mod. Phys. A 36, 2150197 (2021).
  33. M. Ablikim et al. (BESIII Collaboration), Measurement of the cross sections for e+e−→ηπ+π− at center-of-mass energies between 2.00 and 3.08 GeV, Phys. Rev. D 108, L111101 (2023).
  34. M. Ablikim et al. (BESIII Collaboration), Measurement of the Born cross sections for e+e−→η′π+π− at center-of-mass energies between 2.00 and 3.08 GeV, Phys. Rev. D 103, 072007 (2021).
  35. Q. S. Zhou, Z. Y. Bai, H. Xu, J. Z. Wang, and X. Liu, Decoding the role of ρ mesonic states for elucidating the e+e−→a2(1320)π data and other reactions, Phys. Rev. D 112, 074021 (2025).
  36. L. M. Wang, S. Q. Luo, and X. Liu, Light unflavored vector meson spectroscopy around the mass range of 2.4–3 GeV and possible experimental evidence, Phys. Rev. D 105, 034011 (2022).
  37. M. Ablikim et al. (BESIII Collaboration), Measurement of the e+e−→pp¯π0 cross section at s=2.1000–3.0800  GeV, Phys. Rev. D 110, 052006 (2024).
  38. M. N. Achasov, A. Y. Barnyakov, K. I. Beloborodov, A. V. Berdyugin, D. E. Berkaev, A. G. Bogdanchikov, A. A. Botov, T. V. Dimova, V. P. Druzhinin, V. B. Golubev et al., Updated measurement of the e+e−→ωπ0→π0π0γ cross section with the SND detector, Phys. Rev. D 94, 112001 (2016).
  39. B. Aubert et al. (BABAR Collaboration), The e+e−→2(π+π−)π0, 2(π+π−)η, K+K−π+π−π0 and K+K−π+π−η cross sections measured with initial-state radiation, Phys. Rev. D 76, 092005 (2007); 77, 119902(E) (2008).
  40. J. P. Lees et al. (BABAR Collaboration), Study of the reactions e+e−→K+K−π0π0π0, e+e−→KS0K±π∓π0π0, and e+e−→KS0K±π∓π+π− at center-of-mass energies from threshold to 4.5 GeV using initial-state radiation, Phys. Rev. D 107, 072001 (2023).
  41. B. Ketzer, B. Grube, and D. Ryabchikov, Light-meson spectroscopy with COMPASS, Prog. Part. Nucl. Phys. 113, 103755 (2020); 128, 104000(E) (2023).
  42. L. Y. Xiao, X. Z. Weng, X. H. Zhong, and S. L. Zhu, A possible explanation of the threshold enhancement in the process e+e−→ΛΛ¯, Chin. Phys. C 43, 113105 (2019).
  43. Z. Y. Bai, Q. S. Zhou, and X. Liu, Higher strangeonium decays into light flavor baryon pairs like ΛΛ¯, ΣΣ¯, and ΞΞ¯, Phys. Rev. D 108, 094036 (2023).
  44. H. Xu, J. J. Xie, and X. Liu, Implication of the observed e+e−→pp¯π0 for studying the pp¯→ψ(3770)π0 process, Eur. Phys. J. C 76, 192 (2016).
  45. J. Z. Wang, H. Xu, J. J. Xie, and X. Liu, Production of the charmoniumlike state Y(4220) through the pp¯→Y(4220)π0 reaction, Phys. Rev. D 96, 094004 (2017).
  46. D. Y. Chen, J. He, and X. Liu, Nonresonant explanation for the Y(4260) structure observed in the e+e−→J/ψπ+π− process, Phys. Rev. D 83, 054021 (2011).
  47. D. Guo, J. Shi, I. Strakovsky, and B. S. Zou, Analysis of Σ* via isospin selective reaction KLp→π+Σ0, Phys. Rev. D 112, 034006 (2025).
  48. A. Matsuyama, T. Sato, and T. S. H. Lee, Dynamical coupled-channel model of meson production reactions in the nucleon resonance region, Phys. Rep. 439, 193 (2007).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation