4.7 Article

Spin-adapted open-shell random phase approximation and time-dependent density functional theory. I. Theory

期刊

JOURNAL OF CHEMICAL PHYSICS
卷 133, 期 6, 页码 -

出版社

AMER INST PHYSICS
DOI: 10.1063/1.3463799

关键词

configuration interactions; density functional theory; excited states; mathematical operators; RPA calculations; tensors

资金

  1. National Natural Science Foundation of China [20625311, 20773003]
  2. MOST of China [2006CB601103, 2006AA01A119]

向作者/读者索取更多资源

The spin-adaptation of single-reference quantum chemical methods for excited states of open-shell systems has been nontrivial. The primary reason is that the configuration space, generated by a truncated rank of excitations from only one component of a reference multiplet, is spin-incomplete. Those missing configurations are of higher ranks and can, in principle, be recaptured by a particular class of excitation operators. However, the resulting formalisms are then quite involved and there are situations [e.g., time-dependent density functional theory (TD-DFT) under the adiabatic approximation] that prevent one from doing so. To solve this issue, we propose here a tensor-coupling scheme that invokes all the components of a reference multiplet (i.e., a tensor reference) rather than increases the excitation ranks. A minimal spin-adapted n-tuply excited configuration space can readily be constructed by tensor products between the n-tuple tensor excitation operators and the chosen tensor reference. Further combined with the tensor equation-of-motion formalism, very compact expressions for excitation energies can be obtained. As a first application of this general idea, a spin-adapted open-shell random phase approximation is first developed. The so-called translation rule is then adopted to formulate a spin-adapted, restricted open-shell Kohn-Sham (ROKS)-based TD-DFT (ROKS-TD-DFT). Here, a particular symmetry structure has to be imposed on the exchange-correlation kernel. While the standard ROKS-TD-DFT can access only excited states due to singlet-coupled single excitations, i.e., only some of the singly excited states of the same spin (S-i) as the reference, the new scheme can capture all the excited states of spin S-i-1, S-i, or S-i+1 due to both singlet- and triplet-coupled single excitations. The actual implementation and computation are very much like the (spin-contaminated) unrestricted Kohn-Sham-based TD-DFT. It is also shown that spin-contaminated spin-flip configuration interaction approaches can easily be spin-adapted via the tensor-coupling scheme. (C) 2010 American Institute of Physics. [doi:10.1063/1.3463799]

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