  The CKM angle $\gamma/\phi_{3}$ is the only one that is accessible with tree
level decays in a theoretically clean way such that it provides a precision
test of $CP$ violation in the standard model. The Belle II experiment is a
substantial upgrade of the Belle detector and will operate at the SuperKEKB
asymmetric-energy $e^{+}e^{-}$ collider. The accelerator has already
successfully completed the first phase of commissioning in 2016 and first
$e^{+}e^{-}$ collisions in Belle II happened during April 2018. The design
luminosity of SuperKEKB is 8 $\times$ 10$^{35}$ cm$^{-2}$s$^{-1}$ and the Belle
II experiment aims to record 50 ab$^{-1}$ of data, a factor of 50 more than its
predecessor (Belle). The key method to measure $\phi_{3}$ is through
interference between the $B^- \to D^0 K^-$ and $B^- \to \bar{D^{0}} K^{-}$
decays which occurs if the final state of the charm-meson decay is accessible
to both the $D^0$ and $\bar{D^{0}}$ mesons. To achieve the best sensitivity, a
large variety of $D$ and $B$ decay modes are required, which is possible at the
Belle II experiment as almost any final state can be reconstructed including
those with photons. With the ultimate Belle II data sample of 50 ab$^{-1}$, a
determination of $\phi_{3}$ with a precision of $1^{\circ}$ or better is
foreseen. We explain herein the details of the planned measurements at Belle
II.
