掺杂浓度对掺钡 LaCoO3 纳米结构的结构、光学和磁学特性的影响

Jhelai Sahadevan, Mugesh Madavan, Esakki Muthu Sankaran, Ikhyun Kim, Rajesh Venkatesan, Naiyf S. Alharbi, Jamal M Khaled, Sivaprakash Paramasivam
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摘要

本文报告了 Ba x La1-x CoO3(x = 0、0.05 和 0.1)(LBCO)样品的结构、形态、振动、光学和磁学特性。X 射线衍射显示,样品为单一斜方体相。与 LBCO 相比,LCO 的拉曼信号非常小,LBCO 的拉曼峰在 675 cm-1 以上。波长为 484 cm-1 的波段对应于 E g 弯曲和 Ba-O 拉伸的振动模式。UV-DRS 和光致发光光谱显示了紫外线、可见光和近红外光谱的广泛吸收。表面形貌和 EDAX 光谱证实了材料的均匀尺寸分布和均匀微观结构,其中钡的结构更为稳定。XPS 被用来研究枸杞多糖的化学状态,并在过氧化物化合物中发现了 Co (2p)、La (3d)、O (1s) 和 C (1s) 元素。300 eV 以下的峰值表明表面材料中存在不定碳。XPS 勘测谱元素 La、Ba、Co 和 O 具有各自的结合能。LBCO 在 300 K 时的磁化-磁场依赖性表明,钡插入 LCO 后,LBCO 从顺磁性转变为弱铁磁性。钡大大降低了磁饱和度和矫顽力,影响了磁晶的各向异性和矫顽力场。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Influence of doping concentrations on the structural, optical, and magnetic properties of Ba-doped LaCoO3 nanostructure
In this article we report the structural, morphology, vibrational, optical and magnetic properties of Ba x La1−x CoO3 (x = 0, 0.05, and 0.1) (LBCO) samples. The X-ray diffraction shows that samples are in single rhombohedral phase. The Raman signals of LCO were quite small in comparison to LBCO, which exhibited a Raman peak above 675 cm−1. The band seen with a wavenumber of 484 cm−1 corresponds to the vibrational modes of E g bending and Ba–O stretching. UV–DRS and photoluminescence spectra indicated broad absorption over the ultraviolet, visible, and near-infrared spectrums. Surface morphology and EDAX spectra corroborated the materials homogeneous size distribution and homogenous microstructure, with Ba indicating a more stable structure. XPS was used to study chemical states of LBCO and found Co (2p), La (3d), O (1s), and C (1s) elements in perovskite compounds. A peak beneath 300 eV indicated adventitious carbon on surface materials. XPS survey spectrum elements La, Ba, Co, and O had their own binding energies. The magnetization-field dependency of LBCO at 300 K showed that Ba insertion into the LCO switched it from paramagnetic to weak ferromagnetic. Ba considerably decreased magnetic saturation and coercivity, influencing magneto-crystallites’ anisotropy and coercive field.
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