Effective Core Potentials for calculations of continuum spectra of molecules using the molecular R-matrix method
Zdenek Masin, Jakub Benda, Martin Crhan, Gregory S. J. Armstrong, Anna Nelson, Sebastian Mohr, Jonathan Tennyson
TL;DR
This work introduces a robust implementation of Effective Core Potentials (ECPs) into the molecular R-matrix framework UKRmol+ and the QEC interface, enabling accurate continuum-state calculations for molecules containing heavy elements. By deriving and implementing general expressions for ECP integrals over both Gaussian-type and B-spline orbitals, and by translating B-spline orbitals in momentum space, the approach handles 1-, 2-, and 3-centre integrals essential for scattering and photoionization in the presence of ECPs. The authors demonstrate the method on Br$_2$, SiBr$_4$, WH, and CH$_3$I, showing close agreement with all-electron benchmarks and experiment while enabling calculations that would be impractical with all-electron cores. The work broadens the applicability of molecular scattering calculations to heavy-atom targets, supports energy ranges up to ~100 eV with BTOs, and lays groundwork for future inclusion of spin-orbit ECPs and improved quadrature strategies. Overall, this represents a significant step toward efficient and relativistically informed continuum simulations in molecular systems.
Abstract
Implementation of Effective Core Potentials (ECPs) into the molecular scattering suite UKRmol+ is presented together with a set of calculations for a range of targets relevant for plasma modeling. Continuum description in scattering and photoionization calculations for large targets or high-energy electrons often requires the use of numerical continuum functions and the associated molecular integrals. We derive expressions for ECP integrals over B-spline type orbitals using their momentum-space representation and describe their implementation. Sample calculations are presented for electron collision from bromine molecule (Br$_2$), silicon tetrabromide (SiBr$_4$) and tungsten hydride (WH) as well as photoionisation of methyl iodide (CH$_3$I).
