Abstract:Using numerical calculations and analytic theory, we examine the convergence behavior of Gaussian expansions of several model orbitals. By following the approach of Kutzelnigg, we find that the errors in the energies of the optimal n-term even-tempered Gaussian expansions of s-type, p-type, and d-type exponential orbitals are ε n s ∼ exp(−π(3n) 1/2 ), ε n p ∼ exp(−π(5n) 1/2 ), and ε n d ∼ exp(−π(7n) 1/2 ), respectively. We show that such "root-exponential" convergence patterns are a consequence of the orbital … Show more
“…Studies [69,70] suggest that while the FD approach for transition dipoles shows improved convergence behavior compared to the EV approach, perhaps more so than for Spherically averaged polarizability of water in its equilibrium geometry computed using sum-over-states formula (1) [73]; the experimental value is corrected for vibrational effects [75].…”
Section: Electron Correlation Treatmentmentioning
confidence: 99%
“…the diagonal dipole moments, there are technical issues with their use that still need to be overcome [70,71].…”
Sources of uncertainty are reviewed for calculated atomic and molecular data that are important for plasma modeling: atomic and molecular structure and cross sections for electron-atom, electron-molecule, and heavy particle collisions. We concentrate on model uncertainties due to approximations to the fundamental many-body quantum mechanical equations and we aim to provide guidelines to estimate uncertainties as a routine part of computations of data for structure and scattering.
“…Studies [69,70] suggest that while the FD approach for transition dipoles shows improved convergence behavior compared to the EV approach, perhaps more so than for Spherically averaged polarizability of water in its equilibrium geometry computed using sum-over-states formula (1) [73]; the experimental value is corrected for vibrational effects [75].…”
Section: Electron Correlation Treatmentmentioning
confidence: 99%
“…the diagonal dipole moments, there are technical issues with their use that still need to be overcome [70,71].…”
Sources of uncertainty are reviewed for calculated atomic and molecular data that are important for plasma modeling: atomic and molecular structure and cross sections for electron-atom, electron-molecule, and heavy particle collisions. We concentrate on model uncertainties due to approximations to the fundamental many-body quantum mechanical equations and we aim to provide guidelines to estimate uncertainties as a routine part of computations of data for structure and scattering.
“…Klopper and Kutzelnigg109–111 showed that the energy of a hydrogen atom converges exponentially with the square‐root of the number of Gaussian functions used for expanding the 1s‐orbital, as shown in Eq. (12): …”
Section: Basis Set Convergence Of Independent‐ and Correlated‐electromentioning
Electronic structure methods for molecular systems rely heavily on using basis sets composed of Gaussian functions for representing the molecular orbitals. A number of hierarchical basis sets have been proposed over the last two decades, and they have enabled systematic approaches to assessing and controlling the errors due to incomplete basis sets. We outline some of the principles for constructing basis sets, and compare the compositions of eight families of basis sets that are available in several different qualities and for a reasonable number of elements in the periodic table. C 2012 John Wiley & Sons, Ltd.
“…Given that the fitting errors (Table III) in the gLDA1 functional can be of the order of 0.1 mE h , we aimed to obtain the energies of the n-boxium and n-hookium to within 0.1 mE h of their complete basis set (CBS) limits. This is easily achieved for the HF, LDA1 and gLDA1 energies, because they converge exponentially [90][91][92] with the size M of the one-electron basis, but it is less straightforward for traditional post-HF energies.…”
Section: The Lda1 Glda1 and Glda1 Functionalsmentioning
We introduce a generalization (gLDA) of the traditional Local Density Approximation (LDA) within density functional theory. The gLDA uses both the one-electron Seitz radius rs and a two-electron hole curvature parameter η at each point in space. The gLDA reduces to the LDA when applied to the infinite homogeneous electron gas but, unlike the LDA, it is also exact for finite uniform electron gases on spheres. We present an explicit gLDA functional for the correlation energy of electrons that are confined to a one-dimensional space and compare its accuracy with LDA, second- and third-order Møller-Plesset perturbation energies, and exact calculations for a variety of inhomogeneous systems.
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