Abstract

In Paper I, the performances of pre-screening (PS), extended PS (EPS), and cumulant (CU) approximations to the fourth-order density matrix were examined in the context of second-order N-electron valence state perturbation theory (NEVPT2). It has been found that the CU, PS, and even EPS approximations with loose thresholds may introduce intruder states. In the present work, the origin of these "false intruder" states introduced by approximated density matrices is discussed. Canonical NEVPT2 implementations employ a rank reduction trick. By analyzing its residual error, we find that the omission of the rank reduction leads to a more stable multireference perturbation theory for incomplete active space reference wave functions. Such a full rank (FR)-NEVPT2 formulation is equivalent to the conventional NEVPT2 method for the complete active space self-consistent field/complete active space configuration interaction reference wave function. A major drawback of the FR-NEVPT2 formulation is the necessity of the fifth-order density matrix. To avoid the construction of the high-order density matrices, the combination of the FR-NEVPT2 with the CU approximation is studied. However, we find that the CU approximation remains problematic as it still introduces intruder states. The question of how to robustly and efficiently perform internally contracted multireference perturbation theories with approximate densities remains a challenging field of investigation.

Highlights

  • In recent years, various approximate full configuration interaction (FCI) methods, e.g., the density matrix renormalization group (DMRG) approach,1–3 the selected CI/configuration interaction by perturbation with multiconfigurational zeroth-order wavefunction selected by iterative process (CIPSI),4–12 or the full-CI quantum Monte Carlo (FCIQMC)13 ansatz, have been developed to address problems involving many strongly correlated electrons

  • The origin of the intruder state problem arising from approximate CAS wave functions in the NEVPT2 theory has been investigated

  • It is proven that the rank reduction trick in NEVPT2 can cause artifacts, such as the negative Koopmans energies, when the density matrices are approximated

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Summary

Introduction

Various approximate full configuration interaction (FCI) methods, e.g., the density matrix renormalization group (DMRG) approach, the selected CI/configuration interaction by perturbation with multiconfigurational zeroth-order wavefunction selected by iterative process (CIPSI), or the full-CI quantum Monte Carlo (FCIQMC) ansatz, have been developed to address problems involving many strongly correlated electrons These methods are mostly used as approximate complete active space configuration interaction (CASCI) or complete active space selfconsistent field (CASSCF) engines to tackle systems even with nearly one hundred active orbitals. Some multireference perturbation theories (MRPT) based on the DMRG or FCIQMC reference wave function, including the complete active space second-order perturbation theory (CASPT2) and the second-order N-electron valence state perturbation theory (NEVPT2), have been reported These multireference (MR) correlation approaches usually employ the fully internally contraction (FIC) ansatz for the excited configuration state functions (CSFs) that span the first-order-interacting space (FOIS). As tempting as it is, it is important to develop approximation schemes that avoid the calculation and storage of the fourth and fifth order RDM

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