Womes, ManfredBihler, EckardtEisenmenger, Wolfgang2010-08-032016-03-312010-08-032016-03-311988353180114http://nbn-resolving.de/urn:nbn:de:bsz:93-opus-56032http://elib.uni-stuttgart.de/handle/11682/4966http://dx.doi.org/10.18419/opus-4949The authors present measurements of the maximum displacement at the end of a rectangular high-voltage pulse together with the remanent polarization after the pulse under short-circuit condition as a function of the polarizing pulse end length. The pulse length varied from 10 μs to 100 s, and the field strength ranged from 0.8 MV/cm to 2 MV/cm. The original samples were reversely polarized or unpolarized 12-μm-thick films containing 37% β-material. It is concluded that the cooperative model combined with six-site potential alone cannot explain the observed switching back of the remanent polarization, its delayed development, and the long times necessary for polarization reversal. The results are qualitatively consistent with a model of charge injection and charge trapping at polarized crystallites.eninfo:eu-repo/semantics/openAccessDielektrische Polarisation , Polymerfilm , Polyvinylidenfluorid530conferenceObject2011-11-16