English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Plus monthly

Global: Zendy Tools annual

Global: Zendy Tools monthly

Global: Zendy Free Plan

The processes $e^{+}e^{-} \rightarrow K^{\pm} K^{*\mp}(892)$ and $e^{+}e^{-}\rightarrow \eta \phi(1020)$ are calculated in the framework of the extendedNambu-Jona-Lasinio model. The intermediate vector mesons $\rho(770),\omega(782), \phi(1020)$ and their first radially-excited states are taken intoaccount. The obtained results are in satisfactory agreement with theexperimental data. The predictions for the cross sections of the reactions$e^{+}e^{-} \rightarrow K^{\pm} K^{*\mp}(1410)$, $e^{+}e^{-} \rightarrow\eta^{'}(958) \phi(1020)$ and $e^{+}e^{-} \rightarrow \eta \phi(1680)$ weremade.

international journal of modern physics a

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