Phenomenological model of chiral polar smectics is introduced with interact
ions up to the fourth neighboring layers. The minimization of the free ener
gy gives three stable structures: the ferroelectric Sm C* phase, the antife
rroelectric Sm C-A* phase and the hellicoidally modulated structure of the
Sm C-H* phase. The Sm C-H* phase can be recognized as the Sm C-alpha*, phas
e below Sm A phase and as the Sm C-FI2* phase or as the Sm C-FI1* phase whe
n appearing between the Sm C* phase and the Sm C-A* phase. Stability of the
se phases is analyzed and the phase diagram in the space of model parameter
s is presented.