Ordejón Belén, Seijo Luis, Barandiarán Zoila
Departamento de Química, C-XIV, Universidad Autónoma de Madrid, 28049 Madrid, Spain.
J Chem Phys. 2007 May 21;126(19):194712. doi: 10.1063/1.2736703.
Excitons trapped at impurity centers in highly ionic crystals were first described by McClure and Pedrini [Phys. Rev. B 32, 8465 (1985)] as excited states consisting of a bound electron-hole pair with the hole localized on the impurity and the electron on nearby lattice sites, and a very short impurity-ligand bond length. In this work the authors present a detailed microscopic characterization of impurity-trapped excitons in U(4+)-doped Cs(2)GeF(6). Their electronic structure has been studied by means of relativistic ab initio model potential embedded cluster calculations on (UF(6))(2-) and (UF(6)Cs(8))(6+) clusters embedded in Cs(2)GeF(6), in combination with correlation methods based on multireference wave functions. The local geometry of the impurity-trapped excitons, their potential energy curves, and their multielectronic wave functions have been obtained as direct, nonempirical results of the methods. The calculated excited states appear to be significantly delocalized outside the UF(6) volume and their U-F bond length turns out to be very short, closer to that of a pentavalent uranium defect than to that of a tetravalent uranium defect. The wave functions of these excited states show a dominant U 5f(1)7s(1) configuration character. This result has never been anticipated by simpler models and reveals the unprecedented ability of diffuse orbitals of f-element impurities to act as electron traps in ionic crystals.
麦克卢尔和佩德林尼 [《物理评论B》32, 8465 (1985)] 首次描述了高离子晶体中杂质中心捕获的激子,其为一种激发态,由一个束缚的电子 - 空穴对组成,空穴定域在杂质上,电子在附近的晶格位置上,且杂质 - 配体键长非常短。在这项工作中,作者对U(4+)掺杂的Cs₂GeF₆中杂质捕获的激子进行了详细的微观表征。他们通过对嵌入Cs₂GeF₆中的(UF₆)₂⁻和(UF₆Cs₈)⁶⁺团簇进行相对论性从头算模型势嵌入团簇计算,并结合基于多参考波函数的关联方法,研究了其电子结构。杂质捕获激子的局部几何结构、势能曲线和多电子波函数已作为这些方法的直接、非经验性结果获得。计算得到的激发态似乎在UF₆体积之外有显著的离域,并且其U - F键长非常短,更接近五价铀缺陷的键长,而不是四价铀缺陷的键长。这些激发态的波函数显示出占主导的U 5f¹7s¹组态特征。这一结果从未被更简单的模型所预测到,并且揭示了f元素杂质的弥散轨道在离子晶体中作为电子陷阱的前所未有的能力。