  The exclusive photoproduction of upsilon states $\Upsilon(1S)$ and its
radially excited states $\Upsilon(2S,3S)$ is investigated in the context of
ultra-peripheral collisions at the LHC energies. Predictions are presented for
their production in proton-proton, proton-nucleus and nucleus-nucleus collision
at the energies available at the LHC run 2. The rapidity and transverse
momentum distributions are shown, and the robustness of the model is tested
against the experimental results considering $\psi(1S,2S)$ and $\Upsilon(1S)$
states. The theoretical framework considered in the analysis is the light-cone
color dipole formalism, which includes consistently parton saturation effects
and nuclear shadowing corrections.
