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通过太赫兹时域光谱法测量钴掺杂对正铁酸镥电导率的有效控制。

Effective control of conductivity in lutetium orthoferrite with cobalt doping measured by terahertz time-domain spectroscopy.

作者信息

Li Gaofang, Liu Rongyang, Huang Jingguo, Cui Haoyang, Xia Nenghong, Wang Zhi, Huang Zhiming, Chu Junhao

出版信息

Opt Express. 2025 Feb 10;33(3):4127-4137. doi: 10.1364/OE.543028.

DOI:10.1364/OE.543028
PMID:40797738
Abstract

The effective control of conductivity in LuFeO (LFO) with Co doping is explored by terahertz (THz) time-domain spectroscopy. It is demonstrated that the conductivity of 5% Co-doped LFO (LFO:Co 5%) is lower than that of LFO, while that of 15% Co-doped LFO (LFO:Co 15%) is significantly higher than LFO. Furthermore, LFO exhibits two lattice vibration peaks at 0.58 and 1.61 THz, LFO:Co 5% shows only one lattice vibration peak at 1.61 THz, while no distinct vibration peak is observed in LFO:Co 15%. The disappearance of lattice vibration at 0.58 THz is attributed to the shortened Fe (Co)-O bond length resulting from Co doping, thus suppressing magnetic resonance effect of Fe. With 15% Co doping, structural stability is enhanced, and the asymmetric vibration of Lu at surface/interface/boundary is suppressed, resulting in the disappearance of vibration peak at 1.61 THz. The conductivity of LFO:Co 5% is lower than that of LFO, mainly because the lattice vibration at 1.61 THz and oxygen vacancy defects introduced by doping jointly increase the degree of carrier back-scattering, which decreases carrier movement, while the enhancement of conductivity by electronegativity at 5% Co doping is very limited. The significantly higher conductivity of LFO:Co 15% compared to LFO is due to the obvious increase in overall electronegativity and suppression of lattice vibration by 15% Co doping, thereby improving carrier mobility. The insights of this investigation provide important experimental data and theoretical basis for design and production of high-conductivity and stable solid oxide fuel cells cathode.

摘要

通过太赫兹(THz)时域光谱研究了钴掺杂对LuFeO(LFO)电导率的有效控制。结果表明,5%钴掺杂的LFO(LFO:Co 5%)的电导率低于LFO,而15%钴掺杂的LFO(LFO:Co 15%)的电导率显著高于LFO。此外,LFO在0.58和1.61 THz处有两个晶格振动峰,LFO:Co 5%仅在1.61 THz处有一个晶格振动峰,而LFO:Co 15%中未观察到明显的振动峰。0.58 THz处晶格振动的消失归因于钴掺杂导致Fe(Co)-O键长缩短,从而抑制了Fe的磁共振效应。15%钴掺杂时,结构稳定性增强,表面/界面/边界处Lu的不对称振动受到抑制,导致1.61 THz处的振动峰消失。LFO:Co 5%的电导率低于LFO,主要是因为1.61 THz处的晶格振动和掺杂引入的氧空位缺陷共同增加了载流子背散射程度,降低了载流子迁移率,而5%钴掺杂时电负性增强对电导率的提升非常有限。LFO:Co 15%的电导率显著高于LFO,是由于15%钴掺杂使整体电负性明显增加并抑制了晶格振动,从而提高了载流子迁移率。本研究的见解为高电导率和稳定的固体氧化物燃料电池阴极的设计和生产提供了重要的实验数据和理论依据。

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