In a liquid crystalline side chain polyacrylate containing one center of chirality in the terminal alkyl chain of the mesogenic part, switching times of 200–400 μs were measured in the SmC* phase. Below this phase an unidentified phase exists, which shows electroclinic‐like switching. The phase transition between those two phases can be shifted by applying an electric field.
At higher molecular weights three subphases emerge in the SmC* region. Variation of the spacer length revealed, for the first time, ferroelectric switching even at a spacer length of only two CH2 groups.
By shifting the centre of chirality into the spacer of the side group a polymer resulted, which shows electroclinic switching in the SmC* phase, changing to ferroelectric switching when the voltage is increased.
Incorporation of an oxirane ring as chiral building block into the spacer yielded a polymer that shows a sign inversion of the spontaneous polarization in the SmC* phase.
A polymer containing a dioxolane carbonic ester as chiral unit exhibits three switching states, with the third state existing at a low or zero electric field. This phenomenon is known for antiferroelectric liquid crystals.
By doping a racemic LC polymer with a chiral monomeric LC we induced a spontaneous polarization. Colored FLC polymers were obtained by two different approaches. In an FLC–dye copolymer, increasing switching speed in three different chiral smectic phases was observed when increasing the dye concentration.