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The available data on the $Q^2$ dependence of the $\gamma\gamma*(Q^2)\toK\bar K\pi$ reaction cross section in the energy region 1.35-1.55 GeV isexplained by the $\eta(1475)$ resonance production in contrast to theirconventional interpretation with the use of the $f_1(1420)$ resonance. Itresolves theoretically the contradiction between the suppression of the$\eta(1475)\to\gamma\gamma$ decay width and the strong couplings of the$\eta(1475)$ to the $\rho\rho$, $\omega\omega$, and $\gamma\rho^0$ channels.The experimental check of our explanation requires definition of thespin-parity of the resonance contributions, $R$, in $\gamma\gamma*(Q^2)\to R\toK\bar K\pi$ and in $J/\psi\to\gammaR\to\gamma\gamma(\rho^0, \phi)$. This willhelp to solve difficulties accumulated in understanding properties of the$\eta(1475)$ state and its nearest partners.

\eta(1475) and f_1(1420) resonances in \gamma\gamma* collisions and J/\psi\to\gamma(\rho\rho, \gamma\rho^0, \gamma\phi) decays