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Accurate singlet-triplet gaps in biradicals via the spin averaged anti-Hermitian contracted Schrodinger equation

机译:通过旋转平均抗封闭型抗封闭式契约Schrodinger方程精确单态 - 三重态间隙

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摘要

The accurate description of biradical systems, and in particular the resolution of their singlet-triplet gaps, has long posed a major challenge to the development of electronic structure theories. Biradicaloid singlet ground states are often marked by strong correlation and, hence, may not be accurately treated by mainstream, single-reference methods such as density functional theory or coupled cluster theory. The anti-Hermitian contracted Schrodinger equation (ACSE), whose fundamental quantity is the two-electron reduced density matrix rather than the N-electron wave function, has previously been shown to account for both dynamic and strong correlations when seeded with a strongly correlated guess from a complete active space (CAS) calculation. Here, we develop a spin-averaged implementation of the ACSE, allowing it to treat higher multiplicity states from the CAS input without additional state preparation. We apply the spin-averaged ACSE to calculate the singlet-triplet gaps in a set of small main group biradicaloids, as well as the organic four-electron biradicals trimethylenemethane and cyclobutadiene, and naphthalene, benchmarking the results against other state-of-the-art methods reported in the literature.
机译:双自由基系统的精确描述,尤其是其单重态-三重态间隙的解析,长期以来一直是电子结构理论发展的一个重大挑战。双自由度单重态基态通常具有很强的相关性,因此,主流的单参考方法,如密度泛函理论或耦合簇理论,可能无法准确地处理。反厄米收缩薛定谔方程(ACSE)的基本量是双电子约化密度矩阵,而不是N电子波函数,以前已经证明,当使用完全活动空间(CAS)计算中的强相关猜测时,它既可以解释动态关联,也可以解释强关联。在这里,我们开发了一个自旋平均的ACSE实现,允许它处理来自CAS输入的更高多重性状态,而无需额外的状态准备。我们应用自旋平均ACSE计算了一组小的主族双自由基化合物,以及有机四电子双自由基三甲撑甲烷、环丁二烯和萘中的单重态-三重态间隙,并将结果与文献中报道的其他最新方法进行了对比。

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