The changes in the crystalline structure and molecular mobility in the semi-crystalline vinylidene fluoride (VDF) and trifluoroethylene (TrFE) copolymer P(VDF 75 /TrFE 25 ) caused by the ferroelectric-paraelectric phase transition were analyzed using variable temperature solid-state 19 F magic angle spinning (MAS) and 1 H-19 F cross polarization/MAS nuclear magnetic resonance spectroscopy in the temperature range of 42-129 1C. The conformational exchange between trans and gauche at the VDF and VDF-TrFE head-to-head linkage gradually increases at temperatures above 77 1C, and the conformational exchange at the head-to-tail linkage has a key role in the ferroelectric-paraelectric phase transition. The anomalous decrease in the amorphous peak intensities and the presence of a T 1q F value similar to that of the crystalline domain at 122 1C indicate that cooperative motion occurs in both phases just above the transition temperature (T c ). The amorphous domain is assimilated by the crystalline domain upon lowering the temperature from 129 to 85 1C, which significantly increases the crystallinity to below T c , as indicated by the shape of the spectra, and identical T 1q
INTRODUCTIONVinylidene fluoride (VDF)-trifluoroethylene (TrFE) copolymer (P(VDF x /TrFE 1 Àx )), where x is the VDF molar fraction, is a typical ferroelectric polymer that shows a ferroelectric-paraelectric phase transition, which has garnered much interest in the effort to clarify its mechanism. 1,2 Two types of ferroelectric phases have been reported at room temperature, that is, the low-temperature (LT) and the cooled phase, depending on the VDF content and preparation conditions of the copolymer. 2 In the LT phase, the CF 2 dipoles are arranged in parallel because of the planar zigzag formed by the all-trans polymer chains, which is the same arrangement as the PVDF form I (b-form), whereas in the cooled phase, long trans segments are connected by irregular trans-gauche linkages along their chain axis to form a type of super lattice. However, the stable crystal structure in the hightemperature (paraelectric) phase is hexagonal and is composed of statistically mixed chains with TG þ , TG -, T 3 G þ and T 3 Gconformations. These chains rotate about their axes via the onedimensional diffusion of the conformational defects along the chain.Several reports have shown that lamellar crystals grow in P(VDF/ TrFE) films at VDF contents of x ¼ 0.60 to 0.82 when annealed at temperatures above the Curie point (T c ). In particular, annealing such polymers at elevated temperatures in the paraelectric phase increases the integrated X-ray diffraction intensities of the 110 and 200 reflections, which correspond to the all-trans chains, and sharpen the differential scanning calorimetry (DSC) endotherms observed at T c . [3][4][5][6][7] The efficient growth of lamellar crystals in the paraelectric phase has been explained using a sliding diffusion model for the polymer chains. For instance, a polyethylene lamellar crystal can thicken at higher pressures through th...