Site-selective $d^{10}$/$d^0$ substitution in a $S = 1/2$ spin ladder Ba$_2$CuTe$_{1-x}$W$_x$O$_6$ ($0 \leq x \leq 0.3$)
Inorganic Chemistry 61, 4033-4045 (2022) 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 orbita...
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Zusammenfassung: | Inorganic Chemistry 61, 4033-4045 (2022) 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. |
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DOI: | 10.48550/arxiv.2108.02761 |