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, Li1.56Co0.71P2S6 and Li2.26Fe0.94P2S6. The previously unreported Li1.56Co0.71P2S6 crystallizes
in the trigonal space group P31m with lattice parameters a =
6.0193(6) Å and c = 6.5675(9) Å. The CoS6 octahedra are arranged in a honeycomb lattice and form 2D
layers separated by lithium cations. The previously solved Li2.26Fe0.94P2S6 is isostructural
to Li1.56Co0.71P2S6 but
displays site mixing between the Li+ and Fe2+ cations within the thiophosphate layer. Unusually, Li1.56Co0.71P2S6 appears to have P2S63– and not P2S64– 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
Li1.56Co0.71P2S6 and Li2.26Fe0.94P2S6 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) μB, which may be best described by an S + L model, where S =
2 and L = 2, or close to the free ion limit. In the
cobalt thiophosphate, we found the effective moment to be 4.35(2)
μB, which would point to an S = 3/2 and L = 1 model due to octahedral
crystal-field splitting.