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Fundamentals of Ferroelectric Materials 铁电材料基础
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH1
L. Kong, Haitao Huang, Sean Li
Ferroelectricity is defined as the property of a material, with two characteristics, i.e. (i) spontaneous polarization is present and (ii) it is reversible when subjected to external electric fields [1]. The property was first observed in Rochelle salt and is named so because of its analogy to ferromagnetism, which is a magnetic property of a material that has a permanent magnetic moment [2, 3]. Other similarities include hysteresis loop, Curie temperature (TC), domains, and so on. The prefix, ferro, meaning iron (Fe), was used at that time because of the presence of the element in the magnetic materials. However, ferroelectricity has nothing to do with Fe. Even though some ferroelectric materials contain Fe, it is not the originating factor. Generally, as a material is polarized by an external electric field, the induced polarization (P) is linearly proportional to the magnitude of the applied external electric field (E), which is known as dielectric polarization. Above the Curie temperature TC, ferroelectric materials are at a paraelectric state. In this case, a nonlinear polarization is present versus an external electric field. As a result, electric permittivity, according to the slope of the polarization curve, is not a constant. At the ferroelectric state, besides the nonlinearity, a spontaneous nonzero polarization was present, as the applied field (E) is zero. Because the spontaneous polarization can be reversed by a sufficiently strong electric field, it is dependent on the currently applied electric field and the history as well, thus leading to the presence of the hysteresis loop. The electric dipoles in a ferroelectric material are coupled to the crystal lattice of the material, so that the variation in lattice could change the strength of the dipoles, i.e. the strength of the spontaneous polarization. The change in the spontaneous polarization, in turn, leads to a change in the surface charge, which causes
铁电性定义为材料的性质,具有两个特征,即:(i)存在自发极化,(ii)在外加电场作用下可逆[1]。这种性质最早是在Rochelle盐中观察到的,之所以这样命名,是因为它与铁磁性相似,铁磁性是具有永久磁矩的材料的磁性[2,3]。其他相似之处还包括磁滞回线、居里温度(TC)、磁域等。前缀,ferro,意思是铁(Fe),在当时被使用,因为元素存在于磁性材料中。然而,铁电性与铁无关。尽管有些铁电材料含有铁,但它并不是产生铁电的因素。一般来说,当材料被外加电场极化时,感应极化(P)与外加电场(E)的大小成线性比例,称为介电极化。在居里温度TC以上,铁电材料处于准电状态。在这种情况下,一个非线性极化是存在于一个外电场。因此,根据极化曲线的斜率,电介电常数不是常数。在铁电态,除了非线性外,当外加电场(E)为零时,还存在自发的非零极化。由于自发极化可以被足够强的电场逆转,因此它依赖于当前施加的电场和历史,从而导致磁滞回线的存在。铁电材料中的电偶极子与材料的晶格耦合,晶格的变化会改变偶极子的强度,即自发极化的强度。自发极化的变化反过来又引起表面电荷的变化,从而引起
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引用次数: 2
Ferroelectrics in Photocatalysis 光催化中的铁电体
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH9
Liang Fang, L. You, Jun-ming Liu
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引用次数: 16
First-Principles Calculations on Ferroelectrics for Energy Applications 铁电体在能源应用中的第一性原理计算
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH10
G. Jiang, Weijin Chen, Yue Zheng
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引用次数: 1
Dielectric Ceramics and Films for Electrical Energy Storage 用于电能存储的介电陶瓷和薄膜
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH5
Xihong Hao
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引用次数: 3
Ferroelectric Polymer Materials for Electric Energy Storage 用于储能的铁电聚合物材料
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH6
Z. Dang, M. Zheng, J. Zha
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引用次数: 2
Future Perspectives 未来的视角
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.ch11
Haitao Huang
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引用次数: 0
Ferroelectrics in Electrocaloric Cooling 电热冷却中的铁电体
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH8
Biaolin Peng, Qi Zhang
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引用次数: 0
Organic-Inorganic Hybrid Perovskites for Solar Energy Conversion 太阳能转换用有机-无机杂化钙钛矿
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH4
Peng You, Feng Yan
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引用次数: 0
Piezoelectric Energy Generation 压电发电
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.CH2
H. Yeo, S. Trolier-McKinstry
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引用次数: 1
Ferroelectric Photovoltaics 铁电光电
Pub Date : 2018-09-08 DOI: 10.1002/9783527807505.ch3
A. Bhatnagar
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引用次数: 8
期刊
Ferroelectric Materials for Energy Applications
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