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New and Efficient Implementation of CC3
[Image: see text] We present a new and efficient implementation of the closed shell coupled cluster singles and doubles with perturbative triples method (CC3) in the electronic structure program e(T). Asymptotically, a ground state calculation has an iterative cost of 4n(V)(4)n(O)(3) floating point...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American
Chemical Society
2020
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8016187/ https://www.ncbi.nlm.nih.gov/pubmed/33263255 http://dx.doi.org/10.1021/acs.jctc.0c00686 |
Sumario: | [Image: see text] We present a new and efficient implementation of the closed shell coupled cluster singles and doubles with perturbative triples method (CC3) in the electronic structure program e(T). Asymptotically, a ground state calculation has an iterative cost of 4n(V)(4)n(O)(3) floating point operations (FLOP), where n(V) and n(O) are the number of virtual and occupied orbitals, respectively. The Jacobian and transpose Jacobian transformations, required to iteratively solve for excitation energies and transition moments, both require 8n(V)(4)n(O)(3) FLOP. We have also implemented equation of motion (EOM) transition moments for CC3. The EOM transition densities require recalculation of triples amplitudes, as n(V)(3)n(O)(3) tensors are not stored in memory. This results in a noniterative computational cost of 10n(V)(4)n(O)(3) FLOP for the ground state density and 26n(V)(4)n(O)(3) FLOP per state for the transition densities. The code is compared to the CC3 implementations in CFOUR, DALTON, and PSI4. We demonstrate the capabilities of our implementation by calculating valence and core excited states of l-proline. |
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