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赤铁矿FeO中极化子的实空间研究。

Real-space investigation of polarons in hematite FeO.

作者信息

Redondo Jesus, Reticcioli Michele, Gabriel Vit, Wrana Dominik, Ellinger Florian, Riva Michele, Franceschi Giada, Rheinfrank Erik, Sokolović Igor, Jakub Zdenek, Kraushofer Florian, Alexander Aji, Belas Eduard, Patera Laerte L, Repp Jascha, Schmid Michael, Diebold Ulrike, Parkinson Gareth S, Franchini Cesare, Kocan Pavel, Setvin Martin

机构信息

Department of Surface and Plasma Science, Faculty of Mathematics and Physics, Charles University, 180 00 Prague, Czech Republic.

Institute of Applied Physics, TU Wien, 1040 Vienna, Austria.

出版信息

Sci Adv. 2024 Nov;10(44):eadp7833. doi: 10.1126/sciadv.adp7833. Epub 2024 Nov 1.

Abstract

In polarizable materials, electronic charge carriers interact with the surrounding ions, leading to quasiparticle behavior. The resulting polarons play a central role in many materials properties including electrical transport, interaction with light, surface reactivity, and magnetoresistance, and polarons are typically investigated indirectly through these macroscopic characteristics. Here, noncontact atomic force microscopy (nc-AFM) is used to directly image polarons in FeO at the single quasiparticle limit. A combination of Kelvin probe force microscopy (KPFM) and kinetic Monte Carlo (KMC) simulations shows that the mobility of electron polarons can be markedly increased by Ti doping. Density functional theory (DFT) calculations indicate that a transition from polaronic to metastable free-carrier states can play a key role in migration of electron polarons. In contrast, hole polarons are significantly less mobile, and their hopping is hampered further by trapping centers.

摘要

在可极化材料中,电子电荷载流子与周围离子相互作用,导致准粒子行为。由此产生的极化子在许多材料特性中起着核心作用,包括电传输、与光的相互作用、表面反应性和磁阻,并且通常通过这些宏观特性间接研究极化子。在此,非接触原子力显微镜(nc-AFM)用于在单准粒子极限下直接成像FeO中的极化子。开尔文探针力显微镜(KPFM)和动力学蒙特卡罗(KMC)模拟相结合表明,通过Ti掺杂可显著提高电子极化子的迁移率。密度泛函理论(DFT)计算表明,从极化子态到亚稳态自由载流子态的转变在电子极化子迁移中起关键作用。相比之下,空穴极化子的迁移率明显较低,并且它们的跳跃会因陷阱中心而进一步受阻。

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