posted on 2021-07-07, 13:33authored byTimothy
J. Diethrich, Peter Y. Zavalij, Stephanie Gnewuch, Efrain E. Rodriguez
Transition-metal thiophosphates and selenophosphates are layered
systems with the potential for displaying two-dimensional (2D) magnetic
phenomena. We present the crystal structures and magnetic properties
of two lithium transition-metal thiophosphates, Li<sub>1.56</sub>Co<sub>0.71</sub>P<sub>2</sub>S<sub>6</sub> and Li<sub>2.26</sub>Fe<sub>0.94</sub>P<sub>2</sub>S<sub>6</sub>. The previously unreported Li<sub>1.56</sub>Co<sub>0.71</sub>P<sub>2</sub>S<sub>6</sub> crystallizes
in the trigonal space group <i>P</i>31<i>m</i> with lattice parameters <i>a</i> =
6.0193(6) Å and <i>c</i> = 6.5675(9) Å. The CoS<sub>6</sub> octahedra are arranged in a honeycomb lattice and form 2D
layers separated by lithium cations. The previously solved Li<sub>2.26</sub>Fe<sub>0.94</sub>P<sub>2</sub>S<sub>6</sub> is isostructural
to Li<sub>1.56</sub>Co<sub>0.71</sub>P<sub>2</sub>S<sub>6</sub> but
displays site mixing between the Li<sup>+</sup> and Fe<sup>2+</sup> cations within the thiophosphate layer. Unusually, Li<sub>1.56</sub>Co<sub>0.71</sub>P<sub>2</sub>S<sub>6</sub> appears to have P<sub>2</sub>S<sub>6</sub><sup>3–</sup> and not P<sub>2</sub>S<sub>6</sub><sup>4–</sup> anions. We therefore term it a “noninnocent”
anion because of the ambiguous nature of its oxidation state. Combined
neutron diffraction and magnetization measurements reveal that both
Li<sub>1.56</sub>Co<sub>0.71</sub>P<sub>2</sub>S<sub>6</sub> and Li<sub>2.26</sub>Fe<sub>0.94</sub>P<sub>2</sub>S<sub>6</sub> display magnetic
anisotropy as well as no long-range magnetic order down to 5 K. In
the iron thiophosphate, susceptibility indicates an effective moment
of 5.44(3) μ<sub>B</sub>, which may be best described by an <i>S</i> + <i>L</i> model, where <i>S</i> =
2 and <i>L</i> = 2, or close to the free ion limit. In the
cobalt thiophosphate, we found the effective moment to be 4.35(2)
μ<sub>B</sub>, which would point to an <i>S</i> = <sup>3</sup>/<sub>2</sub> and <i>L</i> = 1 model due to octahedral
crystal-field splitting.