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首页> 外文期刊>Macromolecules >Layer-thinning effects on ferroelectricity and the ferroelectric-to-paraelectric phase transition of vinylidene fluoride-trifluoroethylene copolymer layers
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Layer-thinning effects on ferroelectricity and the ferroelectric-to-paraelectric phase transition of vinylidene fluoride-trifluoroethylene copolymer layers

机译:层变薄对偏二氟乙烯-三氟乙烯共聚物层的铁电和铁电-顺电相变的影响

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Dielectric and electromechanical properties of vinylidene fluoride-trifluoroethylene copolymer layers with thickness ranging from 1300 nm down to 65 nm have been investigated by dielectric spectroscopy and electromechanical interferometry. The effects of layer thickness (h) on ferroelectricity and the ferroelectric-to-paraelectric phase transition are discussed on the basis of the temperature (T) dependence of the dielectric constant (epsilon) and electrostrictive and inverse-piezoelectric effects. In the region of h less than a few hundred nanometers, the layer-thinning effect on epsilon becomes prominent, and epsilon decreases with a decrease in h, but the phase transition temperature (T-c) and the Curie constants are not significantly influenced by layer thinning. The dependence of the electrostriction on the square of the applied electric field for unpoled films is nonlinear in the ferroelectric phase, while it is linear in the paraelectric phase. The degree of the nonlinearity decreases as the layer becomes thinner, and for a 65 nm thick film the nonlinearity almost vanishes at temperatures fairly below T-c. Remanent polarizations (P-r) achieved by poling are ca. 55 mC/m(2) for the films of h greater than or equal to 90 nm, while P-r for the 65 nm thick film (40 mC/m(2)) is definitely lower. Differential scanning calorimetry shows that the degree of crystallinity (fraction of ferroelectric crystalline phase) decreases with reduction in film thickness, and especially the crystallinity for the 65 nm thick film is much lower than those for the thicker ones. In comparison, between the 1300 and 65 nm thick films, the reduction in the degree of crystallinity is comparable to the decrease in P-r. The variation of the dielectric constant and the degree of crystallinity on h are reasonably well explained assuming the presence of a nonferroelectric amorphous-like surface near layer. Electron microscopic studies of the 65 nm thick layer suggest a preferred orientation of the chain axis of the crystallites parallel to the film surface. The presence of the preferential crystalline orientation might as well explain the appreciably different values of the surface near layer thickness (12 and 27 nm) evaluated from the h dependence of the dielectric constant and the degree of crystallinity. The layer thickness dependence of the dielectric and electromechanical properties is interpreted as a result of a combined effect of the reduction in degree of crystallinity and the specific crystallite orientation due to layer thinning. [References: 44]
机译:已经通过介电谱和机电干涉法研究了厚度为1300nm至65nm的偏二氟乙烯-三氟乙烯共聚物层的介电和机电性能。基于介电常数(ε)对温度(T)的依赖性以及电致伸缩和反压电效应,讨论了层厚(h)对铁电和铁电-顺电相变的影响。在小于几百纳米的h区域,对epsilon的层变薄效应变得显着,而epsilon随着h的减少而减小,但是相变温度(Tc)和居里常数不受层变薄的影响。对于未极化膜,电致伸缩对施加电场的平方的依赖性在铁电相中是非线性的,而在顺电相中则是线性的。非线性程度随层变薄而降低,对于65 nm厚的薄膜,非线性程度在相当低于T-c的温度下几乎消失。通过极化实现的剩余极化强度(P-r)约为。 h大于或等于90 nm的膜为55 mC / m(2),而65 nm厚的膜(40 mC / m(2))的P-r肯定更低。差示扫描量热法显示,结晶度(铁电结晶相的分率)随着膜厚的减少而降低,特别是65nm厚的膜的结晶度比厚膜的结晶度低得多。相比之下,在1300和65 nm厚的薄膜之间,结晶度的降低与P-r的降低相当。假设存在非铁电非晶态表面附近层,则可以很好地解释介电常数和h上的结晶度的变化。对65nm厚的层的电子显微镜研究表明,微晶链轴平行于膜表面的优选取向。优先晶体取向的存在也可以解释由介电常数的h依赖性和结晶度所评估的表面附近层厚度(12和27nm)的明显不同的值。介电性能和机电性能的层厚度依赖性被解释为由于层变薄导致结晶度降低和特定微晶取向降低的综合作用的结果。 [参考:44]

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