Effect of synthesis conditions and composition on structural and phase states and electrical properties of nanogranular (FeCoZr)x (PZT)100-x films (30 ≤ x ≤ 85 at.%)

J. Fedotova
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Abstract

Granular films containing Fe50Co50Zr10 alloy nanoparticles inside Pb0,81Sr0,04(Na0,5Bi0,5)0,15(Zr0,575Ti0,425)O3 (PZT) ferroelectric matrix possess a combination of functional magnetic and electrical properties which can be efficiently controlled by means of external electric or magnetic fields. The formation of the required granular structure in PZT matrix is only possible if synthesis is carried out in an oxygen-containing atmosphere leading to substantial oxidation of metallic nanoparticles. Thus an important task is to study the oxidation degree of metallic nanoparticles depending on synthesis conditions and the effect of forming phases on the electrical properties of the films. The relationship between the structural and phase state and electrical properties of granular FeCoZr)x (PZT)100-x films (30 ≤ x ≤ 85 at.%) synthesized in an oxygen-containing atmosphere at the oxygen pressure PO in a range of (2.4–5.0) · 10–3 Pa has been studied using X-ray diffraction, EXAFS and four-probe electrical resistivity measurement. Integrated comparative analysis of the structural and phase composition and local atomic order in (FeCoZr)x (PZT)100-x films has for the first time shown the fundamental role of oxygen pressure PO during synthesis on nanoparticle oxidation and phase composition. We show that the oxygen pressure being within PO = 3.2 · 10–3 Pa an increase in x leads to a transition from nanoparticles of Fe(Co,Zr)O complex oxides to a superposition of complex oxides and a-FeCo(Zr,O) ferromagnetic nanoparticles (or their agglomerations). At higher oxygen pressures РО = 5.0 · 10–3 Pa the nanoparticles undergo complete oxidation with the formation of the (FexCo1-x)1-δO complex oxide having a Wurtzite structure. The forming structural and phase composition allows one to explain the observed temperature dependences of the electrical resistivity of granular films. These dependences are distinguished by a negative temperature coefficient of electrical resistivity over the whole range of film compositions at a high oxygen pressure (РО = 5.0 · 10–3 Pa) and a transition to a positive temperature coefficient of electrical resistivity at a lower oxygen pressure (РО = 3.2 · 10–3 Pa) in the synthesis atmosphere and x > 69 at.% in the films. The transition from a negative to a positive temperature coefficient of electrical resistivity which suggests the presence of a metallic contribution to the conductivity is in full agreement with the X-ray diffraction and EXAFS data indicating the persistence of unoxidized a-FeCo(Zr,O) ferromagnetic nanoparticles or their agglomerations.
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合成条件和组成对纳米颗粒(FeCoZr)x (PZT)100-x薄膜(30≤x≤85 at.%)结构、相态和电学性能的影响
在pb0,81sr0,04 (na0,5bi0,5)0,15(Zr0,575Ti0,425)O3 (PZT)铁电基体中含有Fe50Co50Zr10合金纳米颗粒的颗粒膜具有功能磁性和电学性质,可以通过外加电场或磁场有效地控制。PZT基体中所需颗粒结构的形成只有在含氧大气中进行合成才能导致金属纳米颗粒的大量氧化。因此,研究金属纳米颗粒在不同合成条件下的氧化程度以及形成相对薄膜电性能的影响是一项重要的任务。采用x射线衍射、EXAFS和四探针电阻率测量等方法,研究了在含氧气氛下,在(2.4-5.0)·10-3 Pa的氧压PO范围内合成的FeCoZr (PZT)100-x颗粒状薄膜(30≤x≤85 at.%)的结构、相态和电学性能之间的关系。通过对(FeCoZr)x (PZT)100-x薄膜结构、相组成和局部原子序的综合对比分析,首次揭示了合成过程中氧压PO对纳米颗粒氧化和相组成的影响。我们发现,当氧压在PO = 3.2·10-3 Pa范围内时,x的增加会导致Fe(Co,Zr)O络合物氧化物纳米粒子向复合氧化物和a- feco (Zr,O)铁磁性纳米粒子(或它们的团块)的叠加转变。在较高的氧压РО = 5.0·10-3 Pa下,纳米颗粒完全氧化,形成具有纤锌矿结构的(FexCo1-x)1-δO络合物氧化物。形成结构和相组成允许人们解释观察到的颗粒膜电阻率的温度依赖性。在高氧压(РО = 5.0·10-3 Pa)下,薄膜组成的整个范围内的电阻率温度系数为负,而在合成气氛中,在低氧压(РО = 3.2·10-3 Pa)下,电阻率温度系数转变为正,且x > 69。在电影中。从负到正的电阻率温度系数的转变表明存在金属对电导率的贡献,这与x射线衍射和EXAFS数据完全一致,表明未氧化的a- feco (Zr,O)铁磁性纳米颗粒或它们的团块的存在。
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