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Ferroelectric domain wall relaxation in Ba0.25Sr0.75TiO3 films displaying Curie-Weiss behavior

机译:Ba0.25Sr0.75TiO3薄膜中显示居里-魏斯行为的铁电畴壁弛豫

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Ferroelectric films may be used in integrated circuits for high frequency and memory applications. Losses and interfaces between films and electrodes are problematic. This work concerns the temperature and electric field response of the complex dielectric permittivity and the relaxation of domain walls in a ferroelectric layer that is of sufficient quality to show a Curie-Weiss behavior. Laser ablation was used to deposit 1200 nm thick Ba0.25Sr0.75TiO3 layers between metallic oxide, (100 nm) SrRuO3 and (120 nm) La0.67Ca0.33MnO3, films in epitaxial heterostructures. The electric field response (Eless than or equal to80 kV/cm) of the real epsilon(') and imaginary epsilon(') parts of the complex permittivity of the intermediate Ba0.25Sr0.75TiO3 layer in these parallel plane film capacitors was studied at temperatures above and below the phase transition point T-Curie. The latter was determined from the temperature dependence of the inverse dielectric permittivity and its value, T-Curie=145 K, agrees well with that of bulk single crystal. epsilon(') of the Ba0.25Sr0.75TiO3 layer could be suppressed about 80% by a field E=80 kV/cm at temperatures close to T(Curie)epsilon(')(T,E) and epsilon(')(T,E) curves were used to gain insight into the relaxation dynamics of ferroelectric domain walls (DW) in the Ba0.25Sr0.75TiO3 layer. Their influence on epsilon(') was noticed up to T=230 K, well above T-Curie. The most probable relaxation time tau of the DW in Ba0.25Sr0.75TiO3 follows a relation tau=tau(0) exp[(phi-betarootE)/kT], where tau(0)=1.2x10(-10) s phi=75-105 meV, and beta=4.7x10(-24) J m(1/2) V-1/2. (C) 2004 American Institute of Physics.
机译:铁电膜可以用于高频和存储器应用的集成电路中。薄膜和电极之间的损耗和界面是有问题的。这项工作涉及复介电常数的温度和电场响应以及铁电层中畴壁的弛豫,其质量足以显示居里-魏斯行为。激光烧蚀用于在外延异质结构的金属氧化物(100 nm)SrRuO3和(120 nm)La0.67Ca0.33MnO3膜之间沉积1200 nm厚的Ba0.25Sr0.75TiO3层。研究了在这些平行平面薄膜电容器中中间Ba0.25Sr0.75TiO3层的复介电常数的真实epsilon(')和虚构epsilon(')部分的电场响应(E≤80 kV / cm)。温度高于和低于相变点T-居里。后者是由反介电常数的温度依赖性确定的,其值T-Curie = 145 K与块状单晶的值非常吻合。在接近T(居里)的情况下,电场E = 80 kV / cm可以将Ba0.25Sr0.75TiO3层的ε抑制约80%(ε,ε,T,E)和ε( T,E)曲线用于深入了解Ba0.25Sr0.75TiO3层中铁电畴壁(DW)的弛豫动力学。直到T = 230 K时,它们对epsilon(')的影响才显着,远高于T-Curie。 Ba0.25Sr0.75TiO3中DW的最可能弛豫时间tau遵循关系tau = tau(0)exp [(phi-betarootE)/ kT],其中tau(0)= 1.2x10(-10)s phi = 75-105 meV,且beta = 4.7x10(-24)J m(1/2)V-1 / 2。 (C)2004美国物理研究所。

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