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Self-propagating high-temperature synthesis of chromium substituted lanthanum orthoferrites LaFe1-xCrxO3 (0 <= x <= 1)

机译:自蔓延高温合成铬取代镧正铁氧体LaFe1-xCrxO3(0 <= x <= 1)

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摘要

Pure and chromium substituted lanthanum orthoferrites LaFe1-xCrxO3 (x=0, 0.1, 0.25, 0.4, 0.55, 0.7, 0.85, 1) were synthesised in air by self-propagating high-temperature synthesis (SHS): a combustion process involving the reaction of lanthanum(III) oxide, iron(III) oxide, chromium(III) oxide and iron (or chromium) metal powder. Two series of samples were produced: series 1 - SHS in the absence of an external magnetic field; and series 2 - SHS in a magnetic field of 1.1 T; both processes were followed by sintering at 1400 degreesC for 36 h with intermediate grinding. Scanning electron microscopy, energy dispersive analysis of X-rays, X-ray powder diffraction, infra-red and ultra-violet/visible spectroscopy experiments were carried out on both series of samples. X-Ray diffraction data showed that single phase orthorhombic ferrites were produced. The ferrites showed a systematic decrease in lattice parameters and unit cell volume with chromium content (e.g. for series 1: x = 0, V = 242.4 Angstrom (3); x = 1, V = 234.0 Angstrom (3)). Fe-57 Mossbauer spectroscopy indicated that at low Cr concentration (x = 0.1 and 0.25) more than 96% of the Fe atoms experienced a perturbative disruption to their interatomic exchange interactions, consistent with the random distribution of Cr3+ ions on the B sublattice. The remaining 4% or less of Fe atoms were observed in a paramagnetic state, indicating a small degree of inhomogeneous Cr clustering in the lattice. The room temperature exchange interaction percolation limit for Cr substitution of the Fe lattice was found to lie between x = 0.4 and 0.55, and the Mossbauer spectra for the x greater than or equal to 0.55 samples showed paramagnetic singlets. Room temperature magnetisation versus field curves showed hysteresis loops for x less than or equal to 0.7 (series 1) and x less than or equal to 0.55 (series 2), and anhysteretic curves for higher Cr contents. After an initial decrease with increasing Cr, the maximum magnetisations of the samples peaked at x = 0.25 (sigma (max) = 2.1 emu g(-1), series 1) and x = 0.4 (sigma (max) = 1.7 emu g(-1), series 2), before falling to near zero at higher concentrations. These features are consistent with a more homogeneous Cr substitution of the Fe sublattice in the series 2 samples, related to higher diffusion rates during the hotter combustion reactions achieved in the applied field SHS reactions. These results indicate that the SHS route is a potentially useful means of synthesising orthoferrites with desirable properties. [References: 19]
机译:通过自蔓延高温合成(SHS)在空气中合成纯和铬取代的镧系正铁氧体LaFe1-xCrxO3(x = 0,0.1,0.25,0.4,0.55,0.7,0.85,1):涉及反应的燃烧过程包括氧化镧(III),氧化铁(III),氧化铬(III)和铁(或铬)金属粉末。产生了两个系列的样品:系列1-在没有外部磁场的情况下进行SHS;和系列2-在1.1 T磁场中的SHS;在这两个过程之后,均需在1400℃下烧结36小时,同时进行中间研磨。在这两个系列样品上均进行了扫描电子显微镜,X射线能量色散分析,X射线粉末衍射,红外和紫外/可见光谱实验。 X射线衍射数据表明,产生了单相正交铁素体。铁素体显示出随铬含量的晶格参数和晶胞体积的系统性降低(例如对于系列1:x = 0,V = 242.4埃(3); x = 1,V = 234.0埃(3))。 Fe-57 Mossbauer光谱表明,在低Cr浓度(x = 0.1和0.25)下,超过96%的Fe原子对其原子间的相互作用发生扰动破坏,这与Cr 3+离子在B亚晶格上的随机分布相一致。在顺磁性状态下观察到剩余的4%或更少的Fe原子,表明晶格中少量的不均匀Cr聚集。发现Fe晶格取代Cr的室温交换相互作用渗滤极限在x = 0.4和0.55之间,并且x大于或等于0.55的样品的Mossbauer光谱显示顺磁性单重态。室温磁化强度与磁场曲线显示x小于或等于0.7(系列1)和x小于或等于0.55(系列2)的磁滞回线,以及较高Cr含量的磁滞曲线。随着Cr的增加初始降低后,样品的最大磁化强度在x = 0.25(sigma(max)= 2.1 emu g(-1),系列1)和x = 0.4(sigma(max)= 1.7 emu g( -1),系列2),然后在较高浓度下降至接近零。这些特征与在系列2样品中Fe亚晶格中更均匀的Cr替代相一致,这与在应用的现场SHS反应中实现的较热燃烧反应过程中的较高扩散速率有关。这些结果表明,SHS途径是合成具有理想性能的正铁氧体的潜在有用手段。 [参考:19]

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