Exploring the Influence of (n-1)d Subvalence Correlation and of Spin-Orbit Coupling on Chalcogen Bonding

TL;DR

This study uses computational methods to analyze how subvalence (n-1)d correlation and spin-orbit coupling influence chalcogen bonding, revealing their significant and sometimes opposing effects on interaction energies and stability.

Contribution

It provides a detailed computational analysis of the roles of (n-1)d subvalence correlation and spin-orbit coupling in chalcogen bonding, highlighting their relative importance and effects.

Findings

(n-1)d correlation decreases interaction energies in chalcogen bonds.

Spin-orbit coupling effects are comparable to (n-1)d correlation for Te complexes.

SOC2 stabilizes monomers more than dimers, reducing binding.

Abstract

This article presents a comprehensive computational investigation into chalcogen bonding interactions, focusing specifically on elucidating the role of subvalence (n$-$1)d and (n$-$1)sp correlation. The incorporation of inner-shell (n$-$1)d correlation leads to a decrease in interaction energies for chalcogen-bonded systems (at least those studied herein), contradicting the observations regarding halogen bonding documented by Kesharwani et al. in \textit{J. Phys. Chem. A}, \textbf{2018}, 122 (8), 2184-2197. The significance of (n$-$1)sp subvalence correlation appears to be lower by an order of magnitude. Notably, among the various components of interaction energies computed at the PNO-LCCSD(T) or DF-CCSD levels, we identify the PNO-LMP2 or DF-MP2 component of the (n$-$1)d correlation as predominant. Furthermore, we delve into the impact of second-order spin-orbit coupling (SOC2) on these interactions. Specifically, for the Te complexes, SOC2 effects rival (n$-$1)d correlation in importance; for the Se complexes, SOC2 is much less important. Generally, SOC2 stabilizes monomers more than dimers, resulting in reduced binding of the latter. Notably, at equilibrium and stretched geometries, SOC2 and (n$-$1)d destabilize the complex; however, at compressed geometries, they exhibit opposing effects, with (n$-$1)d becoming stabilizing.