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The processes $e^{+} e^{-} \to K^{\pm} (K^{* \mp} (892), K^{* \mp} (1410))$ $e^{+} e^{-} \to K^{\pm} (K^{* \mp} (892), K^{* \mp} (1410))$ and $e^{+} e^{-} \to (η, η^{'} (958)) (ϕ (1020), ϕ (1680))$ in the extended Nambu–Jona-Lasinio model

Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna 141980, Russian Federation, Russia

E-mail Address: volkov@theor.jinr.ru

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and

A. A. Pivovarov

Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna 141980, Russian Federation, Russia

E-mail Address: tex_k@mail.ru

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https://doi.org/10.1142/S0217751X16501554Cited by:3 (Source: Crossref)

Abstract

The processes $e^{+} e^{-} \to K^{\pm} K^{* \mp} (892)$ and $e^{+} e^{-} \to η ϕ (1020)$ are calculated in the framework of the extended Nambu–Jona-Lasinio model. The intermediate vector mesons $ρ (770)$ , $ω (782)$ , $ϕ (1020)$ and their first radially excited states are taken into account. The obtained results are in satisfactory agreement with the experimental data. The predictions for the cross-sections of the reactions $e^{+} e^{-} \to K^{\pm} K^{* \mp} (1410)$ , $e^{+} e^{-} \to η^{'} (958) ϕ (1020)$ and $e^{+} e^{-} \to η ϕ (1680)$ were made.

Keywords:

PACS: 13.66.Bc

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