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A Jeziorski-Monkhorst fully uncontracted multi-reference perturbative treatment. I. Principles second-order versions and tests on ground state potential energy curves

机译:Jeziorski-Monkhorst完全未签订合同的多参考微扰治疗。一原理二阶形式和基态势能曲线测试

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摘要

The present paper introduces a new multi-reference perturbation approach developed at second order, based on a Jeziorski-Mokhorst expansion using individual Slater determinants as perturbers. Thanks to this choice of perturbers, an effective Hamiltonian may be built, allowing for the dressing of the Hamiltonian matrix within the reference space, assumed here to be a CAS-CI. Such a formulation accounts then for the coupling between the static and dynamic correlation effects. With our new definition of zeroth-order energies, these two approaches are strictly size-extensive provided that local orbitals are used, as numerically illustrated here and formally demonstrated in the . Also, the present formalism allows for the factorization of all double excitation operators, just as in internally contracted approaches, strongly reducing the computational cost of these two approaches with respect to other determinant-based perturbation theories. The accuracy of these methods has been investigated on ground-state potential curves up to full dissociation limits for a set of six molecules involving single, double, and triple bond breaking together with an excited state calculation. The spectroscopic constants obtained with the present methods are found to be in very good agreement with the full configuration interaction results. As the present formalism does not use any parameter or numerically unstable operation, the curves obtained with the two methods are smooth all along the dissociation path.
机译:本文介绍了一种基于Jeziorski-Mokhorst展开式(使用单个Slater行列式作为扰动器)的二阶多参考扰动方法。由于这种干扰选择,可以建立有效的哈密顿量,允许在参考空间(此处假定为CAS-CI)内修整哈密顿量矩阵。然后,这种表述考虑了静态和动态相关效应之间的耦合。根据我们对零阶能量的新定义,这两种方法严格地在尺寸上是扩展的,前提是要使用局部轨道,如此处的数字所示并在上正式演示。同样,与内部收缩方法一样,本形式主义允许对所有双激励算子进行因式分解,从而相对于其他基于行列式的摄动理论,极大地降低了这两种方法的计算成本。这些方法的准确性已在基态电势曲线上进行了研究,该曲线对于一组包含单键,双键和三键断裂以及激发态计算的六个分子的完全解离极限。发现用本方法获得的光谱常数与完整构型相互作用结果非常吻合。由于当前的形式主义不使用任何参数或数值上不稳定的操作,因此使用这两种方法获得的曲线在整个解离路径上都是平滑的。

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