Abstract

In chemistry, stereochemically active lone pairs are typically described as an important non-bonding effect, and recent interest has centred on understanding the derived effect of lone pair expression on physical properties such as thermal conductivity. To manipulate such properties, it is essential to understand the conditions that lead to lone pair expression and provide a quantitative chemical description of their identity to allow comparison between systems. Here, density functional theory calculations are used first to establish the presence of stereochemically active lone pairs on antimony in the archetypical chalcogenide MnSb2O4. The lone pairs are formed through a similar mechanism to those in binary post-transition metal compounds in an oxidation state of two less than their main group number [e.g. Pb(II) and Sb(III)], where the degree of orbital interaction (covalency) determines the expression of the lone pair. In MnSb2O4 the Sb lone pairs interact through a void space in the crystal structure, and their their mutual repulsion is minimized by introducing a deflection angle. This angle increases significantly with decreasing Sb-Sb distance introduced by simulating high pressure, thus showing the highly destabilizing nature of the lone pair interactions. Analysis of the chemical bonding in MnSb2O4 shows that it is dominated by polar covalent interactions with significant contributions both from charge accumulation in the bonding regions and from charge transfer. A database search of related ternary chalcogenide structures shows that, for structures with a lone pair (SbX 3 units), the degree of lone pair expression is largely determined by whether the antimony-chalcogen units are connected or not, suggesting a cooperative effect. Isolated SbX 3 units have larger X-Sb-X bond angles and therefore weaker lone pair expression than connected units. Since increased lone pair expression is equivalent to an increased orbital interaction (covalent bonding), which typically leads to increased heat conduction, this can explain the previously established correlation between larger bond angles and lower thermal conductivity. Thus, it appears that for these chalcogenides, lone pair expression and thermal conductivity may be related through the degree of covalency of the system.

Highlights

  • Active lone pairs are usually treated as textbook examples of non-bonding effects and occur in posttransition metal compounds in which the post-transition metal is in an oxidation state of two lower than its main group number, such as Pb(II) and Sb(III)

  • 482 Tolborg et al Expression and interactions of stereochemically active lone pairs established framework, with some complexity induced by the presence of the transition metal causing, for example, the different oxygen atoms to behave quite differently

  • We have shown that MnSb2O4 has all the characteristics of a material with Sb(III) stereochemically active lone pairs

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Summary

Introduction

Active lone pairs are usually treated as textbook examples of non-bonding effects and occur in posttransition metal compounds in which the post-transition metal is in an oxidation state of two lower than its main group number, such as Pb(II) and Sb(III) This means that the two outermost s electrons are available to form a lone pair, leading to, after hybridization, the possibility of an asymmetric coordination environment. And still in most textbooks, stereochemically active lone pairs are described as on-site sp hybridization on the metal atom, which is the origin of its name as a ‘chemically inactive’ (i.e. non-bonding) but ‘stereochemically active’ (i.e. structure-determining) effect This does not fully explain the anion dependence on the tendency to form an asymmetric coordination environment. We report a characterization of all other bonding interactions in the material, and we perform a database analysis on a group of related structures in order to derive general features regarding the influence of stereochemically active lone pairs on crystal structures, and their relation to physical properties, thermal conductivity

Computational details
Density of states and valence electron density
Real space identification of the lone pairs
Pressure effects on lone pair interaction
Topological analysis of the electron density
 10À4
Implications for other materials with stereochemically active lone pairs
Conclusions
Funding information
Full Text
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