2017
DOI: 10.1063/1.4976130
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Automatic active space selection for the similarity transformed equations of motion coupled cluster method

Abstract: An efficient scheme for the automatic selection of an active space for similarity transformed equations of motion (STEOM) coupled cluster method is proposed. It relies on state averaged configuration interaction singles (CIS) natural orbitals and makes it possible to use STEOM as a black box method. The performance of the new scheme is tested for singlet and triplet valence, charge transfer, and Rydberg excited states.

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Cited by 63 publications
(78 citation statements)
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“…The process of selecting this active space has already been made automatic using a process based on configuration interaction singles averaged densities. 48 In the present study, the default value (0.01) is used for both the occupied (OTHRESH) and virtual (VTHRESH) active space selection thresholds, in all but one cases. For the system containing a tetrafluor-ethylene and an ethyene molecule separated at 3.5Å, both values are set to 0.001 to reach convergence with respect to the size of the active space.…”
Section: Computational Details 21 Excitation Energy Calculationsmentioning
confidence: 99%
“…The process of selecting this active space has already been made automatic using a process based on configuration interaction singles averaged densities. 48 In the present study, the default value (0.01) is used for both the occupied (OTHRESH) and virtual (VTHRESH) active space selection thresholds, in all but one cases. For the system containing a tetrafluor-ethylene and an ethyene molecule separated at 3.5Å, both values are set to 0.001 to reach convergence with respect to the size of the active space.…”
Section: Computational Details 21 Excitation Energy Calculationsmentioning
confidence: 99%
“…Thus, not all elements in the SD block of trueG^ are zero, although one may hope that the coupling between active and inactive blocks is small, especially if the difference in orbital energies is large. This allows for the automatization of the STEOM active space selection procedure by using state averaged CIS natural orbitals with large occupation numbers . One caveat is that partitioning the orbital spaces into active and inactive parts leads to the loss of unitary invariance, but the impact of this is usually negligible or can be removed by computing more roots .…”
Section: Substantive Modificationsmentioning
confidence: 99%
“…This allows for the automatization of the STEOM active space selection procedure by using state averaged CIS natural orbitals with large occupation numbers . One caveat is that partitioning the orbital spaces into active and inactive parts leads to the loss of unitary invariance, but the impact of this is usually negligible or can be removed by computing more roots . Once trueS^ is obtained, the G SS block can diagonalized which is an operation that scales as O ( N 4 ).…”
Section: Substantive Modificationsmentioning
confidence: 99%
“…The occupied index in the above equation is still in local basis, and one can perform a recanonicalization of the occupied space by diagonalizing the occupied‐occupied block of the Fock matrix. However, the recanonicalization is only important in active space‐based methods like STEOM‐CCSD, and the EOM‐CCSD energies are invariant to it. The advantage of this approach is that one uses a single set of PNOs for the entire calculation, because only the ground state calculation is performed in terms of PNOs and excited state is done in terms of the canonical orbitals.…”
Section: Theory and Computational Detailsmentioning
confidence: 99%