Site-selective $d^{10}$/$d^0$ substitution in a $S = 1/2$ spin ladder Ba$_2$CuTe$_{1-x}$W$_x$O$_6$ ($0 \leq x \leq 0.3$)

TL;DR

This study demonstrates how selective site substitution of $d^{10}$ and $d^0$ cations in a spin ladder perovskite can tune magnetic interactions and suppress magnetic order, revealing potential for engineering exotic quantum magnetic states.

Contribution

It provides experimental evidence that $d^{10}$ and $d^0$ dopants can selectively modify intra-ladder interactions in a spin ladder perovskite, enabling control over magnetic ground states.

Findings

W$^{6+}$ preferentially substitutes Te$^{6+}$ at the corner-sharing site.

Doping suppresses magnetic ordering, similar to spin-liquid behavior.

Selective doping tunes intra-ladder magnetic interactions.

Abstract

Remarkably, doping isovalent $d^{10}$ and $d^0$ cations onto the $B$'' site in $A_2B$'$B$''O$_6$ double perovskites has the power to direct the magnetic interactions between magnetic $B$' cations. This is due to changes in orbital hybridization, which favors different superexchange pathways, and leads to the formation of alternative magnetic structures depending on whether $B$'' is $d^{10}$ or $d^0$. Furthermore, the competition generated by introducing mixtures of $d^{10}$ and $d^0$ cations can drive the material into the realms of exotic quantum magnetism. Here, a W$^{6+}$ $d^0$ dopant was introduced to a $d^{10}$ hexagonal perovskite Ba$_2$CuTeO$_6$, which possesses a spin ladder geometry of Cu$^{2+}$ cations, creating a Ba$_2$CuTe$_{1-x}$W$_x$O$_6$ solid solution ($x$ = 0 - 0.3). Neutron and synchrotron X-ray diffraction show that W$^{6+}$ is almost exclusively substituted for Te$^{6+}$ on the corner-sharing site within the spin ladder, in preference to the face-sharing site between ladders. This means the intra-ladder interactions are selectively tuned by the $d^0$ cations. Bulk magnetic measurements suggest this suppresses magnetic ordering in a similar manner to that observed for the spin-liquid like material Sr$_2$CuTe$_{1-x}$W$_x$O$_6$. This further demonstrates the utility of $d^{10}$ and $d^0$ dopants as a tool for tuning magnetic ground states in a wide range of perovskites and perovskite-derived structures.