European Physical Journal C: Particles and Fields (Nov 2020)
Study of the process $$e^+e^- \rightarrow \eta \pi ^0\gamma $$ e + e - → η π 0 γ in the energy range $$\sqrt{s} = {1.05-2.00}$$ s = 1.05 - 2.00 GeV with the SND detector
- M. N. Achasov,
- A. Yu. Barnyakov,
- A. A. Baykov,
- K. I. Beloborodov,
- A. V. Berdyugin,
- D. E. Berkaev,
- A. G. Bogdanchikov,
- A. A. Botov,
- T. V. Dimova,
- V. P. Druzhinin,
- V. B. Golubev,
- A. N. Kirpotin,
- L. V. Kardapoltsev,
- A. S. Kasaev,
- A. G. Kharlamov,
- I. A. Koop,
- A. A. Korol,
- D. P. Kovrizhin,
- A. S. Kupich,
- K. A. Martin,
- N. A. Melnikova,
- N. Yu. Muchnoy,
- A. E. Obrazovsky,
- E. V. Pakhtusova,
- K. V. Pugachev,
- D. V. Rabusov,
- Yu. A. Rogovsky,
- Y. S. Savchenko,
- A. I. Senchenko,
- S. I. Serednyakov,
- D. N. Shatilov,
- Yu. M. Shatunov,
- D. A. Shtol,
- D. B. Shwartz,
- Z. K. Silagadze,
- I. K. Surin,
- M. V. Timoshenko,
- Yu. V. Usov,
- V. N. Zhabin,
- V. V. Zhulanov
Affiliations
- M. N. Achasov
- Budker Institute of Nuclear Physics, SB RAS
- A. Yu. Barnyakov
- Budker Institute of Nuclear Physics, SB RAS
- A. A. Baykov
- Budker Institute of Nuclear Physics, SB RAS
- K. I. Beloborodov
- Budker Institute of Nuclear Physics, SB RAS
- A. V. Berdyugin
- Budker Institute of Nuclear Physics, SB RAS
- D. E. Berkaev
- Budker Institute of Nuclear Physics, SB RAS
- A. G. Bogdanchikov
- Budker Institute of Nuclear Physics, SB RAS
- A. A. Botov
- Budker Institute of Nuclear Physics, SB RAS
- T. V. Dimova
- Budker Institute of Nuclear Physics, SB RAS
- V. P. Druzhinin
- Budker Institute of Nuclear Physics, SB RAS
- V. B. Golubev
- Budker Institute of Nuclear Physics, SB RAS
- A. N. Kirpotin
- Budker Institute of Nuclear Physics, SB RAS
- L. V. Kardapoltsev
- Budker Institute of Nuclear Physics, SB RAS
- A. S. Kasaev
- Budker Institute of Nuclear Physics, SB RAS
- A. G. Kharlamov
- Budker Institute of Nuclear Physics, SB RAS
- I. A. Koop
- Budker Institute of Nuclear Physics, SB RAS
- A. A. Korol
- Budker Institute of Nuclear Physics, SB RAS
- D. P. Kovrizhin
- Budker Institute of Nuclear Physics, SB RAS
- A. S. Kupich
- Budker Institute of Nuclear Physics, SB RAS
- K. A. Martin
- Budker Institute of Nuclear Physics, SB RAS
- N. A. Melnikova
- Budker Institute of Nuclear Physics, SB RAS
- N. Yu. Muchnoy
- Budker Institute of Nuclear Physics, SB RAS
- A. E. Obrazovsky
- Budker Institute of Nuclear Physics, SB RAS
- E. V. Pakhtusova
- Budker Institute of Nuclear Physics, SB RAS
- K. V. Pugachev
- Budker Institute of Nuclear Physics, SB RAS
- D. V. Rabusov
- Budker Institute of Nuclear Physics, SB RAS
- Yu. A. Rogovsky
- Budker Institute of Nuclear Physics, SB RAS
- Y. S. Savchenko
- Budker Institute of Nuclear Physics, SB RAS
- A. I. Senchenko
- Budker Institute of Nuclear Physics, SB RAS
- S. I. Serednyakov
- Budker Institute of Nuclear Physics, SB RAS
- D. N. Shatilov
- Budker Institute of Nuclear Physics, SB RAS
- Yu. M. Shatunov
- Budker Institute of Nuclear Physics, SB RAS
- D. A. Shtol
- Budker Institute of Nuclear Physics, SB RAS
- D. B. Shwartz
- Budker Institute of Nuclear Physics, SB RAS
- Z. K. Silagadze
- Budker Institute of Nuclear Physics, SB RAS
- I. K. Surin
- Budker Institute of Nuclear Physics, SB RAS
- M. V. Timoshenko
- Budker Institute of Nuclear Physics, SB RAS
- Yu. V. Usov
- Budker Institute of Nuclear Physics, SB RAS
- V. N. Zhabin
- Budker Institute of Nuclear Physics, SB RAS
- V. V. Zhulanov
- Budker Institute of Nuclear Physics, SB RAS
- DOI
- https://doi.org/10.1140/epjc/s10052-020-08556-w
- Journal volume & issue
-
Vol. 80,
no. 11
pp. 1 – 10
Abstract
Abstract The process $$e^+e^-\rightarrow \eta \pi ^0\gamma $$ e + e - → η π 0 γ is studied in the center-of-mass energy range 1.05–2.00 GeV using data with an integrated luminosity of 94.5 $$\hbox {pb}^{-1}$$ pb - 1 collected by the SND detector at the VEPP-2000 $$e^{+}e^{-}$$ e + e - collider. The $$e^+e^-\rightarrow \eta \pi ^0\gamma $$ e + e - → η π 0 γ cross section is measured for the first time. It is shown that the dominant mechanism of this reaction is the transition through the $$\omega \eta $$ ω η intermediate state. The measured cross section of the subprocess $$e^+e^-\rightarrow \omega \eta \rightarrow \eta \pi ^0\gamma $$ e + e - → ω η → η π 0 γ is consistent with previous measurements in the $$e^+e^-\rightarrow \pi ^+\pi ^-\pi ^0\eta $$ e + e - → π + π - π 0 η mode. It is found, with a significance of $$5.6\sigma $$ 5.6 σ , that the process $$e^+e^-\rightarrow \eta \pi ^0\gamma $$ e + e - → η π 0 γ is not completely described by hadronic vector-pseudoscalar intermediate states. The cross section of this missing contribution, which can originate from radiation processes, e. g. $$e^+e^-\rightarrow a_{0}(1450)\gamma $$ e + e - → a 0 ( 1450 ) γ , is measured. It is found to be 15–20 pb in the wide energy range from 1.3 to 1.9 GeV.