Effect of Stereochemically Active Electron Lone Pairs on Magnetic Ordering in Trivanadates

Abstract

Stereoactive electron lone pairs derived from filled 5/6s 2 states of p-block cations are an intriguing electronic and geometric structure motif that have been exploited for diverse applications such as thermoelectrics, thermochromics, photocatalysis, and nonlinear optics. Layered trivanadates are dynamic intercalation hosts, where the insertion of cations can be used to tune electron correlation, charge localization, and magnetic ordering. However, the interaction of 5/6s 2 stereoactive electron lone pairs with layered trivanadates remains unexplored. In this study, we contrast s-and p-block trivanadates and map off-centering in the coordination environment and reduction in symmetry arising from the stereochemical activity of lone pair cations to the emergence of filled antibonding lone-pair 6s 2 −O 2p hybridized states. The former is studied by high-resolution single-crystal X-ray diffraction studies of TlV 3 O 8 and isostructural RbV 3 O 8 to probe distinct differences in Tl and Rb coordination environments and the resulting modulation of V−V interactions in V 3 O 8 slabs. The latter has been probed by variable-energy hard X-ray photoelectron spectroscopy (HAXPES) measurements, which manifest orbital-specific contributions from bonding and antibonding interactions of stereoactive Tl 6s 2 electron lone pairs in TlV 3 O 8 . The spectroscopic assignment of valence band states to stereoactive lone pairs is further corroborated by first-principles electronic structure calculations, crystal orbital Hamilton population analyses, and electron localization function maps. The presence of the Tl 6s 2 electron lone pair in TlV 3 O 8 brings about the off-centering of Tl + cations, which leads to anisotropy in Tl−O bonds. The off-centering of Tl ions weakens V−O bonds in one direction, which subsequently strengthens directional V−V coupling. Magnetic measurements reveal ferromagnetic signatures for both RbV 3 O 8 and TlV 3 O 8 . However, the differences in V•••V interactions significantly affect the energy balance of the superexchange interactions, resulting in an ordering temperature of 140 K for TlV 3 O 8 as compared to 125 K for RbV 3 O 8 . The results demonstrate the distinctive effects of stereochemically active lone pairs in modifying electronic structure near the Fermi level and for mediating superexchange interactions.

Toggling Stereochemical Activity through Interstitial Positioning of Cations between 2D V2O5 Double Layers

“…However, in the case of Tl centers in δ-Tl 0.5 V 2 O 5 , the ELF maps in Figure G–I show greater asymmetry. As observed in HAXPES data, the stabilization of Tl 6s–O 2p AB states mediated by hybridization with Tl 6p as per a second-order Jahn–Teller distortion yields AB Tl 6s, 6p–O 2p lone-pair states at the VBM . Being occupied AB states, they give rise to electron localization in AB orbitals around Tl, which is reflected as depletion of electron density from Tl–O bonds.…”

“…As observed in HAXPES data, the stabilization of Tl 6s–O 2p AB states mediated by hybridization with Tl 6p as per a second-order Jahn–Teller distortion yields AB Tl 6s, 6p–O 2p lone-pair states at the VBM. 41 Being occupied AB states, they give rise to electron localization in AB orbitals around Tl, which is reflected as depletion of electron density from Tl–O bonds. In the ELF map for δ-Pb 0.5 V 2 O 5 , once again, considerable electron depletion from Pb–O bonds is observed, and the ELF is strongly distorted around the Pb centers, denoting strong stereochemical activity of Pb 6s 2 states, as also observed in HAXPES plots and COHP data.…”