  We argue that in the color-flavor-locking (CFL) superconducting phase
classical soliton solutions can exist, whose excitations should be interpreted
as states formed by a quark (or an antiquark) and condensed diquarks. This
finding extends the picture of quark-hadron-continuity showing the existence of
a region, intermediate between the CFL and the hypernuclear phase, where chiral
solitons and Nambu Goldstone bosons can exist. We derive an expression of the
soliton mass in terms of the QCD coupling, $g_s$, and the Nambu Goldstone boson
parameters. From the quark-hadron continuity we can draw an argument in favor
of the interpretation of the $\Theta^+(1540)$ particle in terms of a strange
antiquark and two highly correlated $ud$ pairs (diquarks).
