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Molecular Physics
An International Journal at the Interface Between Chemistry and Physics
Volume 121, 2023 - Issue 11-12: Special Issue of Molecular Physics in Honour of Péter Szalay
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Péter G. Szalay Special Issue of Molecular Physics

Cholesky decomposition of two-electron integrals in quantum-chemical calculations with perturbative or finite magnetic fields using gauge-including atomic orbitals

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Article: e2101562 | Received 14 May 2022, Accepted 07 Jul 2022, Published online: 20 Jul 2022
 

Abstract

A rigorous analysis is carried out concerning the use of Cholesky decomposition (CD) of two-electron integrals in the case of quantum-chemical calculations with finite or perturbative magnetic fields and gauge-including atomic orbitals. We investigate in particular how permutational symmetry can be accounted for in such calculations and how this symmetry can be exploited to reduce the computational requirements. A modified CD procedure is suggested for the finite-field case that roughly halves the memory demands for the storage of the Cholesky vectors. The resulting symmetry of the Cholesky vectors also enables savings in the computational costs. For the derivative two-electron integrals in case of a perturbative magnetic field we derive CD expressions by means of a first-order Taylor expansion of the corresponding finite magnetic-field formulas with the field-free case as reference point. The perturbed Cholesky vectors are shown to be antisymmetric (as already proposed by Burger et al. [ J. Chem. Phys. 155, 074105 (2021)]) and the corresponding expressions enable significant savings in the required integral evaluations (by a factor of about four) as well as in the actual construction of the Cholesky vectors (by means of a two-step procedure similar to the one presented by Folkestad et al. [J. Chem. Phys. 150, 194112 (2019)] and Zhang et al. [J. Phys. Chem. A 125, 4258–4265 (2021)]). Numerical examples with cases involving several hundred basis functions verify our suggestions concerning CD in case of finite and perturbative magnetic fields.

GRAPHICAL ABSTRACT

Acknowledgments

This paper is dedicated to Professor Péter G. Szalay on the occasion of his 60th birthday. One of the authors (J.G.) thanks Péter G. Szalay for more than thirty years of friendship, the hospitality during many visits to Budapest, and collaboration in numerous scientific projects.

Disclosure statement

No potential conflict of interest was reported by the author(s).

Additional information

Funding

The authors acknowledge funding by the Deutsche Forschungsgemeinschaft (DFG) within project B5 of the TRR 146 [project number 233 630 050]. S.S. also acknowledges support from the DFG via [grant number STO 1239/1-1].

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