Effects of Co substitution on the structural and magnetic properties of Sr(Ni1βˆ’x_{1-x}Cox_x)2_2P2_2

Abstract

Although SrNi2_2P2_2 adopts the common ThCr2_2Si2_2 structure for Tβ‰₯325T\geq 325 K, being in an uncollapsed tetragonal (ucT) state, on cooling below 325 K it adopts a one-third collapsed orthorhombic (tcO) phase where one out of every three P-rows bond across the Sr layers. On the other hand, SrCo2_2P2_2 only exhibits the uncollapsed ThCr2_2Si2_2 structure from room temperature down to 1.8 K. Neither SrNi2_2P2_2 nor SrCo2_2P2_2 manifest magnetic transitions down to 50 mK and 2 K, respectively. In this work we report the effects of Co substitution in Sr(Ni1βˆ’x_{1-x}Cox_x)2_2P2_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 xβ‰₯0.1x \geq 0.1. Substitution levels in the range 0.11≀x≀0.580.11\leq x\leq 0.58 show no signs of any transition down to 1.8 K in the magnetization or resistance measurements in the range 1.8Β K≀T≀300Β K1.8\ \text{K}\leq T\leq 300\ \text{K}. However, different magnetically ordered states emerge for xβ‰₯0.65x\geq 0.65, and disappear for xβ‰₯0.99x\geq 0.99, recovering the known paramagnetic properties of the parent compound SrCo2_2P2_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 ThCr2_2Si2_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.Comment: 17 pages, 20 figure

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