The supramolecular material FCH-C3-A is a ferroelectric with two dipolar sublattices, each switching at its own coercive field, and its conductivity depends on the polarization state.
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A supramolecular ferroelectric with two sublattices and polarization dependent conductivity
The supramolecular material FCH-C3-A is a ferroelectric with two dipolar sublattices, each switching at its own coercive field, and its conductivity depends on the polarization state.