  We address the formation of topological edge solitons in rotating
Su-Schrieffer-Heeger waveguide arrays. The linear spectrum of the non-rotating
topological array is characterized by the presence of topological gap with two
edge states residing in it. Rotation of the array significantly modifies the
spectrum and may move these edge states out of the topological gap. Defocusing
nonlinearity counteracts this tendency and shifts such modes back into
topological gap, where they acquire structure of tails typical for topological
edge states. We present rich bifurcation structure for rotating topological
solitons and show that they can be stable. Rotation of the topologically
trivial array, without edge states in its spectrum, also leads to the
appearance of localized edge states, but in a trivial semi-infinite gap.
Families of rotating edge solitons bifurcating from the trivial linear edge
states exist too and sufficiently strong defocusing nonlinearity can also drive
them into the topological gap, qualitatively modifying the structure of their
tails.
