Basis Set Effect on Linear Response Density Functional Theory Calculations on Periodic Systems

23 June 2025, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

In this work, we present an investigation of the role of basis set size on linear response (LR) calculations of electronic properties of extended systems using density functional theory with periodic boundary conditions (DFT-PBC) and Gaussian-type atomic orbital (GTO) bases. We report results of electric dipole-electric dipole polarizability, optical rotation, and electronic excitation energies (computed as poles of the LR function) on a series of 1D and 3D periodic systems. The basis sets employed are based on the Dunning series: cc-pVXZ, with X ranging from double-ζ to quintuple-ζ and include the bases augmented with diffuse functions: aug-cc-pVXZ. The calculations are possible thanks to an extension of the coupled-perturbed Kohn-Sham code in the GAUSSIAN software to work with a different number of orbitals at each k point in reciprocal space, as orbitals with small overlap eigenvalues are projected out during the orthonormalization procedure of the basis set before the self-consistent field procedure used to evaluate the energy. The results on the test systems indicate that large basis sets, including diffuse functions, are necessary to reach quantitative agreement with experimental data and the complete basis set limit for LR properties even at DFT-PBC level.

Keywords

Linear Response
Basis Set Dependence
Density Functional Theory
Periodic Boundary Conditions

Supplementary materials

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Supporting Information
Description
The geometry of the systems considered in this work; the ORD curves for α-quartz; the isotropic α polarizability and OR computed with SVWN5 and HSE06, MVG and LG(OI), and the (aug-)cc-pVXZ basis sets with X = D, T, Q, and 5; the excitation energy values for the first two electronic transitions of polyvinylene; the first two excitation wavelengths (nm) for polyvinylene oligomers up to 14 carbon centers; the excitation energy values for the first two electronic transitions of polyyne in Table S6; multiple excitation wavelengths (nm) of polyyne; and the first two excitation wavelengths (nm) for polyyne oligomers.
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