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arXiv 2209.01577cond-mat.mes-hallcond-mat.str-el
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耦合自旋1/2纳米石墨烯的分子间交换理论

Theory of intermolecular exchange in coupled spin-1/2 nanographenes

David Jacob, Joaquín Fernández-Rossier

摘要:

开壳层纳米石墨烯可以共价键合并且仍然保持它们的局部矩,形成相互作用的自旋晶格。在苯型纳米石墨烯的情况下,Ovchinnikov-Lieb规则预测超结构的基态的自旋,从而预测分子间交换的符号。在这里,我们解决了这种类型的系统中的分子间交换的微观机制。我们发现,在一般情况下,三种不同的机制作出贡献。首先,洪德铁磁交换,促进重叠轨道中电子的铁磁相互作用。第二,分子间杂化驱动的超交换,与Anderson动力学交换相同,它是Hubbard- $U$能量标度的递减函数,并且总是反铁磁的。第三,库仑驱动的超交换,其作为$U$的函数增加,并且涉及在整个结构上延伸的激发分子轨道的虚拟激发。我们发现,库仑驱动的超交换可以是铁或反铁磁,占Ovchinnikov-Lieb规则。我们计算这些交换能的情况下,耦合$S=1/2$ phenalenyl triangulenes,使用多构型的方法都与哈伯德和扩展的哈伯德模型,从而解决的影响,长程库仑相互作用的交换相互作用。

英文摘要:

Open-shell nanographenes can be covalently bonded and still preserve their local moments, forming interacting spins lattices. In the case of benzenoid nanographenes, the Ovchinnikov-Lieb rules anticipate the spin of the ground state of the superstructure, and thereby the sign of the intermolecular exchange. Here we address the underlying microscopic mechanisms for intermolecular exchange in this type of system. We find that, in general, three different mechanisms contribute. First, Hund's ferromagnetic exchange that promotes ferromagnetic interactions of electrons in overlapping orbitals. Second, superexchange driven by intermolecular hybridization, identical to Anderson kinetic exchange, which is a decreasing function of the Hubbard-$U$ energy scale, and is always antiferromagnetic. Third, a Coulomb-driven superexchange, that increases as a function of $U$, and involves virtual excitation of excited molecular orbitals that are extended over the entire structure. We find that Coulomb-driven superexchange can be either ferro or antiferromagnetic, accounting for Ovchinnikov-Lieb rules. We compute these exchange energies for the case of coupled $S=1/2$ phenalenyl triangulenes, using multi-configurational methods both with Hubbard and extended Hubbard models, thereby addressing the influence of long-range Coulomb interactions on the exchange interactions.

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