TY - JOUR
T1 - The origin of the stereochemically active Pb(II) lone pair
T2 - DFT calculations on PbO and PbS
AU - Walsh, Aron
AU - Watson, Graeme W.
PY - 2005/5
Y1 - 2005/5
N2 - The concept of a chemically inert but stereochemically active 6s 2 lone pair is commonly associated with Pb(II). We have performed density functional theory calculations on PbO and PbS in both the rocksalt and litharge structures which show anion dependence of the stereochemically active lone pair. PbO is more stable in litharge while PbS is not, and adopts the symmetric rocksalt structure showing no lone pair activity. Analysis of the electron density, density of states and crystal orbital overlap populations shows that the asymmetric electron density formed by Pb(II) is a direct result of anion-cation interactions. The formation has a strong dependence on the electronic states of the anion and while oxygen has the states required for interaction with Pb 6s, sulphur does not. This explains for the first time why PbO forms distorted structures and possesses an asymmetric density and PbS forms symmetric structures with no lone pair activity. This analysis shows that distorted Pb(II) structures are not the result of chemically inert, sterically active lone pairs, but instead result from asymmetric electron densities that rely on direct electronic interaction with the coordinated anions.
AB - The concept of a chemically inert but stereochemically active 6s 2 lone pair is commonly associated with Pb(II). We have performed density functional theory calculations on PbO and PbS in both the rocksalt and litharge structures which show anion dependence of the stereochemically active lone pair. PbO is more stable in litharge while PbS is not, and adopts the symmetric rocksalt structure showing no lone pair activity. Analysis of the electron density, density of states and crystal orbital overlap populations shows that the asymmetric electron density formed by Pb(II) is a direct result of anion-cation interactions. The formation has a strong dependence on the electronic states of the anion and while oxygen has the states required for interaction with Pb 6s, sulphur does not. This explains for the first time why PbO forms distorted structures and possesses an asymmetric density and PbS forms symmetric structures with no lone pair activity. This analysis shows that distorted Pb(II) structures are not the result of chemically inert, sterically active lone pairs, but instead result from asymmetric electron densities that rely on direct electronic interaction with the coordinated anions.
KW - Density functional theory
KW - Electronic structure
KW - Lead oxide
KW - Lone pairs
UR - http://www.scopus.com/inward/record.url?scp=17644373071&partnerID=8YFLogxK
U2 - 10.1016/j.jssc.2005.01.030
DO - 10.1016/j.jssc.2005.01.030
M3 - Article
AN - SCOPUS:17644373071
SN - 0022-4596
VL - 178
SP - 1422
EP - 1428
JO - Journal of Solid State Chemistry
JF - Journal of Solid State Chemistry
IS - 5
ER -