2021
DOI: 10.1016/j.matt.2021.09.008
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Electrostriction-enhanced giant piezoelectricity via relaxor-like secondary crystals in extended-chain ferroelectric polymers

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Cited by 23 publications
(45 citation statements)
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“…The temperature was controlled using a of coP-52/48QSAP (E C = 21 MV/m). According to recent reports, 21,24,32 the in situ slope at E = 0 [(∂S 1 /∂E)| E=0 ] in the returning S 1 −E loops during high-field (e.g., above the E C at 100 MV/m) bipolar poling could be calculated (Figure 1b,d). In the returning loops, a large in situ remanent polarization (P r ) persists at E = 0.…”
Section: ■ Introductionmentioning
confidence: 88%
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“…The temperature was controlled using a of coP-52/48QSAP (E C = 21 MV/m). According to recent reports, 21,24,32 the in situ slope at E = 0 [(∂S 1 /∂E)| E=0 ] in the returning S 1 −E loops during high-field (e.g., above the E C at 100 MV/m) bipolar poling could be calculated (Figure 1b,d). In the returning loops, a large in situ remanent polarization (P r ) persists at E = 0.…”
Section: ■ Introductionmentioning
confidence: 88%
“…23 Furthermore, if relaxor-like (i.e., highly mobile) secondary crystals (SCs) were induced in the OAF layers (i.e., SC OAF ) of the P(VDF-TrFE) copolymers with an extended-chain crystal (ECC) structure, piezoelectricity was further enhanced via the P r0 -biased electrostriction. 24 For example, the quenched (Q), stretched (S), annealed at 130 °C (A), and electrically poled (P) P(VDF-TrFE) 52/48 mol % copolymer film (coP-52/48QSAP) exhibited a high d 31 of 57.6 ± 2.4 pm/V at room temperature. Note, SCs had been reported before for PVDF polymers 25,26 and were ascribed to the short −(CH 2 CF 2 ) n − sequences separated by head-to-head and tailto-tail (HHTT) defects (usually 5−6 mol %) in PVDF chains.…”
Section: ■ Introductionmentioning
confidence: 99%
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