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

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