Mason Jarrett L, Harb Hassan, Topolski Josey E, Hratchian Hrant P, Jarrold Caroline Chick
Department of Chemistry , Indiana University , 800 East Kirkwood Avenue , Bloomington , Indiana 47405 , United States.
Department of Chemistry and Chemical Biology and Center for Chemical Computation and Theory , University of California, Merced , 5200 North Lake Road , Merced , California 95343 , United States.
Acc Chem Res. 2019 Nov 19;52(11):3265-3273. doi: 10.1021/acs.accounts.9b00474. Epub 2019 Nov 8.
Lanthanide () oxide clusters and molecular systems provide a bottom-up look at the electronic structures of the bulk materials because of close parallels in the patterns of 4f subshell occupancy between the molecular and bulk O size limits. At the same time, these clusters and molecules offer a challenge to the theory community to find appropriate and robust treatments for the 4f patterns across the series. Anion photoelectron (PE) spectroscopy provides a powerful experimental tool for studying these systems, mapping the energies of the ground and low-lying excited states of the neutral relative to the initial anion state, providing spectroscopic patterns that reflect the 4f occupancy. In this Account, we review our anion PE spectroscopic and computational studies on a range of small lanthanide molecules and cluster species. The PE spectra of O ( = Ce, Pr, Sm, Eu) diatomic molecules show spectroscopic signatures associated with detachment of an electron from what can be described as a diffuse 6s-like orbital. While the spectra of all four diatomics share this common transition, the fine structure in the transition becomes more complex with increasing 4f occupancy. This effect reflects increased coupling between the electrons occupying the corelike 4f and diffuse 6s orbitals with increasing . Understanding the PE spectra of these diatomics sets the stage for interpreting the spectra of polyatomic molecular and cluster species. In general, the results confirm that the partial 4f subshell occupancy is largely preserved between molecular and bulk oxides and borides. However, they also suggest that surfaces and edges of bulk materials may support a low-energy, diffuse 6s band, in contrast to bulk interiors, in which the 6s band is destabilized relative to the 5d band. We also identify cases in which the molecular centers have 4f occupancy rather than bulklike 4f, which results in weaker -O bonding. Specifically, Sm centers in mixed Ce-Sm oxides or in SmO ( ≤ ) clusters have this higher 4f occupancy. The PE spectra of these particular species exhibit a striking increase in the relative intensities of excited-state transitions with decreasing photon energy (resulting in lower photoelectron kinetic energy). This is of what is expected on the basis of the threshold laws that govern photodetachment. We relate this phenomenon to strong electron-neutral interactions unique to these complex electronic structures. The time scale of the interaction, which shakes up the electronic configuration of the neutral, increases with decreasing electron momentum. From a computational standpoint, we point out that special care must be taken when considering cluster and molecular systems toward the center of the series (e.g., Sm, Eu), where treatment of electrons explicitly or using an effective core potential can yield conflicting results on competing subshell occupancies. However, despite the complex electronic structures associated with partially filled 4f subshells, we demonstrate that inexpensive and tractable calculations yield useful qualitative insight into the general electronic structural features.
镧系()氧化物团簇和分子体系为研究块体材料的电子结构提供了一种自下而上的视角,因为分子和块体尺寸范围内4f亚壳层占据模式存在紧密的相似性。同时,这些团簇和分子对理论界提出了挑战,要求找到适用于整个系列4f模式的合适且稳健的处理方法。阴离子光电子(PE)能谱为研究这些体系提供了一种强大的实验工具,可绘制中性态相对于初始阴离子态的基态和低激发态的能量,提供反映4f占据情况的能谱模式。在本综述中,我们回顾了对一系列小的镧系分子和团簇物种进行的阴离子PE能谱和计算研究。O(= Ce、Pr、Sm、Eu)双原子分子的PE能谱显示出与从可描述为类似弥散6s轨道的电子脱离相关的能谱特征。虽然所有这四种双原子分子的能谱都有这种共同的跃迁,但随着4f占据度增加,跃迁中的精细结构变得更加复杂。这种效应反映了随着增加,占据类芯4f轨道和弥散6s轨道的电子之间的耦合增强。理解这些双原子分子的PE能谱为解释多原子分子和团簇物种的能谱奠定了基础。总体而言,结果证实分子氧化物和硼化物与块体氧化物和硼化物之间在4f亚壳层的部分占据情况在很大程度上得以保留。然而,结果还表明,与块体内部不同,块体材料的表面和边缘可能支持低能量的弥散6s能带,在块体内部,6s能带相对于5d能带不稳定。我们还确定了一些情况,即分子中心具有4f占据而非块体状的4f,这导致-O键较弱。具体而言,混合Ce-Sm氧化物或SmO(≤)团簇中的Sm中心具有这种较高的4f占据度。这些特定物种的PE能谱显示,随着光子能量降低(导致光电子动能降低),激发态跃迁的相对强度显著增加。这与光解离阈值定律所预期的情况相反。我们将这种现象与这些复杂电子结构特有的强电子-中性相互作用联系起来。相互作用的时间尺度会扰乱中性态的电子构型,随着电子动量降低而增加。从计算角度来看,我们指出,在考虑向系列中心(例如Sm、Eu)的团簇和分子体系时必须格外小心,在这些位置,显式处理电子或使用有效核势可能会在竞争的亚壳层占据情况上产生相互矛盾的结果。然而,尽管与部分填充的4f亚壳层相关的电子结构复杂,但我们证明,廉价且易于处理的计算能够对一般电子结构特征提供有用的定性见解。