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We reinvestigate $K^*\Lambda(1116)$ photoproduction off the nucleon target,based on an effective Lagrangian approach. We include higher nucleon resonancessuch as $N(2000)\, 5/2^+$, $N(2060)\,5/2^-$, $N(2120)\,3/2^-$, and$N(2190)\,7/2^-$, of which the data are taken from the 2012 edition of Reviewof Paritcle Physics, in addition to the $t$-channel diagrams ($K$, $K^*$, and$\kappa$), the $s$-channel nucleon, and $u$-channel hyperon($\Lambda$,$\Sigma$, and $\Sigma^*$) contributions. We find that the $N(2120)\,3/2^-$ and$N(2190)\,7/2^-$ resonances are essential in describing the new CLAS data forcharged $K^*$ photoproduction. On the other hand, they rarely affect forneutral $K^*$ photoproduction.

Effects of $N(2000)\, 5/2^+$, $N(2060)\,5/2^-$, $N(2120)\,3/2^-$, and $N(2190)\,7/2^-$ on $K^*\Lambda$ photoproduction