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A recently proposed local self-interaction correction (LSIC) method [Zope textit{et al.} J. Chem. Phys., 2019,{bf 151}, 214108] when applied to the simplest local density approximation provides significant improvement over standard Perdew-Zunger SIC (PZSIC) for both equilibrium properties such as total or atomization energies as well as properties involving stretched bond such as barrier heights. The method uses an iso-orbital indicator to identify the single-electron regions. To demonstrate the LSIC method, Zope textit{et al.} used the ratio $z_sigma$ of von Weizsacker $tau_sigma^W$ and total kinetic energy densities $tau_sigma$, ($z_sigma = tau_sigma^W/tau_sigma$) as a scaling factor to scale the self-interaction correction. The present work further explores the LSIC method using a simpler scaling factor as a ratio of orbital and spin densities in place of the ratio of kinetic energy densities. We compute a wide array of both, equilibrium and non-equilibrium properties using the LSIC and orbital scaling methods using this simple scaling factor and compare them with previously reported results. Our study shows that the present results with simple scaling factor are comparable to those obtained by LSIC($z_sigma$) for most properties but have slightly larger errors. We furthermore study the binding energies of small water clusters using both the scaling factors. Our results show that LSIC with $z_{sigma}$ has limitation in predicting the binding energies of weakly bonded system due to the inability of $z_{sigma}$ to distinguish weakly bonded region from slowly varying density region. LSIC when used with density ratio as a scaling factor, on the other hand, provides good description of water cluster binding energies, thus highlighting the appropriate choice of iso-orbital indicator.
The Perdew-Zunger (PZ) method provides a way to remove the self-interaction (SI) error from density functional approximations on an orbital by orbital basis. The PZ method provides significant improvements for the properties such as barrier heights o
Semi-local approximations to the density functional for the exchange-correlation energy of a many-electron system necessarily fail for lobed one-electron densities, including not only the familiar stretched densities but also the less familiar but cl
We study the importance of self-interaction errors in density functional approximations for various water-ion clusters. We have employed the Fermi-Lowdin orbital self-interaction correction (FLOSIC) method in conjunction with LSDA, PBE, and SCAN to d
(Semi)-local density functional approximations (DFAs) suffer from self-interaction error (SIE). When the first ionization energy (IE) is computed as the negative of the highest-occupied orbital (HO) eigenvalue, DFAs notoriously underestimate them com
The Perdew-Zunger self-interaction correction(PZ-SIC) improves the performance of density functional approximations(DFAs) for the properties that involve significant self-interaction error(SIE), as in stretched bond situations, but overcorrects for e