  We introduce a new version of $\psi$-Hilfer fractional derivative, on an
arbitrary time scale. The fundamental properties of the new operator are
investigated and, in particular, we prove an integration by parts formula.
Using the Laplace transform and the obtained integration by parts formula, we
then propose a $\psi$-Riemann-Liouville fractional integral on times scales.
The applicability of the new operators is illustrated by considering a
fractional initial value problem on an arbitrary time scale, for which we prove
existence, uniqueness and controllability of solutions in a suitable Banach
space. The obtained results are interesting and nontrivial even for particular
choices: (i) of the time scale; (ii) of the order of differentiation; and/or
(iii) function $\psi$; opening new directions of investigation.
