European Physical Journal C: Particles and Fields (Feb 2022)
Study of the process $$e^+e^- \rightarrow \eta \eta \gamma $$ e + e - → η η γ in the energy range $$\sqrt{s} = \text{1.17--2.00 }$$ s = 1.17--2.00 GeV with the SND detector
- M. N. Achasov,
- A. Yu. Barnyakov,
- K. I. Beloborodov,
- A. V. Berdyugin,
- D. E. Berkaev,
- A. G. Bogdanchikov,
- A. A. Botov,
- T. V. Dimova,
- V. P. Druzhinin,
- 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,
- 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,
- SND Collaboration
Affiliations
- M. N. Achasov
- Budker Institute of Nuclear Physics, SB RAS
- A. Yu. Barnyakov
- 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
- 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
- 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
- SND Collaboration
- DOI
- https://doi.org/10.1140/epjc/s10052-022-10102-9
- Journal volume & issue
-
Vol. 82,
no. 2
pp. 1 – 8
Abstract
Abstract The process $$e^+e^-\rightarrow \eta \eta \gamma $$ e + e - → η η γ is studied in the center-of-mass energy range 1.17–2.00 GeV using data with an integrated luminosity of 201 pb $$^{-1}$$ - 1 collected by the SND detector at the VEPP-2000 $$e^+e^-$$ e + e - collider. The $$e^+e^-\rightarrow \eta \eta \gamma $$ e + e - → η η γ cross section is measured for the first time. It is shown that the dominant mechanism of this reaction is the transition through the $$\phi \eta $$ ϕ η intermediate state. Our result on the $$e^+e^-\rightarrow \eta \eta \gamma $$ e + e - → η η γ cross section is consistent with the $$e^+e^-\rightarrow \phi \eta $$ e + e - → ϕ η measurement in the $$\phi \rightarrow K^+ K^-$$ ϕ → K + K - mode. The search for radiative processes contributing to the $$e^+e^-\rightarrow \eta \eta \gamma $$ e + e - → η η γ cross section is performed, and no significant signal is observed.