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固溶电子-卤铅钙钛矿中的铁电大极化子。

Solvated Electrons in Solids-Ferroelectric Large Polarons in Lead Halide Perovskites.

机构信息

Department of Chemistry, Columbia University, New York, New York 10027, United States.

出版信息

J Am Chem Soc. 2021 Jan 13;143(1):5-16. doi: 10.1021/jacs.0c10943. Epub 2020 Dec 15.

Abstract

Solvation plays a pivotal role in chemistry and biology. A solid-state analogy of solvation is polaron formation, but the magnitude of Coulomb screening is typically an order of magnitude weaker than that of solvation in aqueous solutions. Here, we describe a new class of polarons, the ferroelectric large polaron, proposed initially by Miyata and Zhu in 2018 (Miyata, K.; Zhu, X.-Y. Ferroelectric Large Polarons. 2018, 17 (5), 379-381). This type of polaron allows efficient Coulomb screening of an electron or hole by extended ordering of dipoles from symmetry-broken unit cells. The local ordering is reflected in the ferroelectric-like THz dielectric responses of lead halide perovskites (LHPs) and may be partially responsible for their exceptional optoelectronic performances. Despite the likely absence of long-range ferroelectricity in LHPs, a charge carrier may be localized to and/or induce the formation of nanoscale domain boundaries of locally ordered dipoles. Based on the known planar nature of energetically favorable domain boundaries in ferroelectric materials, we propose that a ferroelectric polaron localizes to planar boundaries of transient polar nanodomains. This proposal is supported by dynamic simulations showing sheet-like transient electron or hole wave functions in LHPs. Thus, the Belgian-waffle-shaped ferroelectric polaron in the three-dimensional LHP crystal structure is a large polaron in two dimensions and a small polaron in the perpendicular direction. The ferroelectric large polaron may form in other crystalline solids characterized by dynamic symmetry breaking and polar fluctuations. We suggest that the ability to form ferroelectric large polarons can be a general principle for the efficient screening of charge carriers from scattering with other charge carriers, with charged defects and with longitudinal optical phonons, thus contributing to enhanced optoelectronic properties.

摘要

溶剂化在化学和生物学中起着关键作用。溶剂化的固态类似物是极化子形成,但库仑屏蔽的幅度通常比水溶液中的溶剂化弱一个数量级。在这里,我们描述了一类新的极化子,即铁电大极化子,最初由 Miyata 和 Zhu 于 2018 年提出(Miyata,K.;Zhu,X.-Y.铁电大极化子。2018,17(5),379-381)。这种极化子允许通过来自对称破缺单元的扩展偶极子有序来有效地屏蔽电子或空穴的库仑。局部有序反映在卤化铅钙钛矿(LHPs)的铁电似太赫兹介电响应中,并且可能部分负责其异常的光电性能。尽管 LHPs 中可能不存在长程铁电性,但载流子可能被局部有序偶极子的纳米级畴边界定位和/或诱导形成。基于铁电材料中有利的能量畴边界的已知平面性质,我们提出一个电荷载流子被定位到瞬态极性纳米畴的平面边界。这一建议得到了动态模拟的支持,该模拟显示了 LHPs 中片状瞬态电子或空穴波函数。因此,在三维 LHP 晶体结构中,比利时华夫饼状的铁电大极化子在二维中是一个大极化子,在垂直方向上是一个小极化子。铁电大极化子可能在其他以动态对称破缺和偶极子波动为特征的晶态固体中形成。我们建议,形成铁电大极化子的能力可以成为从与其他载流子、带电缺陷和纵光学声子的散射中有效屏蔽载流子的一般原则,从而有助于增强光电性能。

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