Target problems
* Linear optical (i.e. electronic) response of molecules or clusters, also second-order nonlinear response. * Non-linear response to classical high-intensity electromagnetic fields, taking into account both the ionic and electronic degrees of freedom. * Ground-state and excited state electronic properties of systems with lower dimensionality, such as quantum dots. * Photo-induced reactions of molecules (e.g., photo-dissociation, photo-isomerization, etc.). * In the immediate future, extension of these procedures to systems that are infinite and periodic in one or more dimensions ( polymers, slabs, nanotubes, solids), and to electronic transport.Theoretical basis
* The underlying theories are DFT and TDDFT. Also, the code may perform dynamics by considering the classical (i.e. point-particle) approximation for the nuclei. These dynamics may be non-adiabatic, since the system evolves following the Ehrenfest path. It is, however, a mean-field approach. * Regarding TDDFT, one can use three different approaches: ** the standard TDDFT-based linear-response theory of Casida, which provides the excitation energies and oscillator strengths for ground-state to excited-state transitions. ** the explicit time-propagation of the TDDFT equations, which allows for the use of large external potentials, well beyond the range of validity of perturbation theory. ** the Sternheimer equation (density-functional perturbation theory) in the frequency domain, using only occupied states.Methodology
* As numerical representation, the code works without a basis set, relying on numerical meshes. Nevertheless, auxiliary basis sets ( plane waves, atomic orbitals) are used when necessary. Recently, the code offers the possibility of working with non-uniform grids, which adapt to the inhomogeneity of the problem, and of making use of multigrid techniques to accelerate the calculations. * For most calculations, the code relies on the use of pseudopotentials of two types: Troullier-Martins, and Hartwigsen-Goedecker-Hutter. * In addition to being able to treat systems in the standard 3 dimensions, 2D and 1D modes are also available. These are useful for studying, e.g., the two-dimensional electron gas that characterizes a wide class of quantum dots.Technical aspects
* The code has been designed with emphasis on parallel scalability. In consequence, it allows for multiple task divisions, this utilises mesh division software,See also
* Quantum chemistry computer programsReferences
External links
* {{DEFAULTSORT:Octopus (software) Computational chemistry software Free science software Software using the GPL license