The dielectric response of the ferroelectric chiral smectic C phase in
a bias electric field is studied theoretically within the Landau mode
l using the constant amplitude approximation. It is argued that the re
sponse consists of two modes, one of which is related to the unwinding
of the helix (the unwinding mode), whereas the other mode is associat
ed with the distortion of the polarization distribution at constant pi
tch of the helix (the Goldstone mode). The relaxation frequency of the
unwinding mode (f(U)), which is inversely proportional to the square
of the sample dimension along the helical axis, is estimated to be of
the order of 10(-4) Hz for a sample of length l almost-equal-to mm alo
ng the helical axis. Consequently, in dielectric experiments performed
usually at frequencies higher than f(U), only the Goldstone mode cont
ribution is detected. In this way, we can explain the behaviour of the
measured static dielectric susceptibility which goes to zero as the c
ritical field is approached from below, although the model predicts th
at the total static dielectric susceptibility, being a sum of the Gold
stone mode and the unwinding mode contribution, diverges at the critic
al field.