Effects of Co substitution on the structural and magnetic properties of Sr(Ni${}_{1-x}$Co${}_x$)${}_2$P${}_2$

Abstract

Although SrNi${}_2$P${}_2$ adopts the common ThCr${}_2$Si${}_2$ structure for $T\ge 325$ K, being in an uncollapsed tetragonal state, on cooling below 325 K it adopts a one-third collapsed orthorhombic phase where one out of every three P rows bond across the Sr layers. On the other hand, SrCo${}_2$P${}_2$ only exhibits the uncollapsed ThCr${}_2$Si${}_2$ structure from room temperature down to 1.8 K. Neither SrNi${}_2$P${}_2$ nor SrCo${}_2$P${}_2$ manifests magnetic transitions down to 50 mK and 2 K, respectively. In this work we report the effects of Co substitution in Sr(Ni${}_{1-x}$Co${}_x$)${}_2$P${}_2$, which allows for tuning the transition between the one-third collapsed and the uncollapsed structure. We find a rapid decrease of the one-third collapsed structural transition temperature with increasing Co fraction, until reaching full suppression for $x\ge 0.1$. Substitution levels in the range $0.11\le x\le 0.58$ show no signs of any transition down to 1.8 K in the magnetization or resistance measurements in the range $1.8\text{K}\le T\le 300\text{K}$. However, different magnetically ordered states emerge for $x\ge 0.65$, and disappear for $x\ge 0.99$, recovering the known paramagnetic properties of the parent compound SrCo${}_2$P${}_2$. These results are summarized in a phase diagram, built upon the characterization done on single crystals with different Co fraction. Both the magnetic and structural properties are compared to other systems with ThCr${}_2$Si${}_2$ structure that exhibit magnetic ordering and collapsed tetragonal transitions. The magnetic ordering and moment formation are well described by Takahashi's spin fluctuation theory of itinerant electron magnetism.

17 pages, 20 figures