2019
DOI: 10.48550/arxiv.1912.07921
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Octopus, a computational framework for exploring light-driven phenomena and quantum dynamics in extended and finite systems

Nicolas Tancogne-Dejean,
Micael J. T. Oliveira,
Xavier Andrade
et al.
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Cited by 2 publications
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“…where ∆Ω = Ω i+1 − Ω i is the step of the discretization. The annihilation and creation operators of the continuum must be transformed back to the operators of the discrete set of modes as: We use a locally modified version of the pseudopotential, real-space DFT code OCTOPUS [66][67][68]. The calculation of electronic excited states via the Casida TDDFT method first requires a converged ground state electronic structure on optimized molecular geometries.…”
Section: Appendix B: Transformation Of Photon Mode Densitymentioning
confidence: 99%
“…where ∆Ω = Ω i+1 − Ω i is the step of the discretization. The annihilation and creation operators of the continuum must be transformed back to the operators of the discrete set of modes as: We use a locally modified version of the pseudopotential, real-space DFT code OCTOPUS [66][67][68]. The calculation of electronic excited states via the Casida TDDFT method first requires a converged ground state electronic structure on optimized molecular geometries.…”
Section: Appendix B: Transformation Of Photon Mode Densitymentioning
confidence: 99%
“…The carrier wavelength λ is 1030 nm. The time-dependent wavefunctions and Hubbard U eff are computed by propagating generalized Kohn-Sham equations within real-time TDDFT+U , as provided by the Octopus package [33][34][35] . We employed the local density approximation for describing the local DFT part, and we computed the effective U eff = U − J for Mo d orbitals, using localized atomic orbitals from Competing Interests The authors declare that they have no competing financial interests.…”
mentioning
confidence: 99%