The compound ${\mathrm{SrNi}}_2{\mathrm{P}}_2$ can exhibit multiple crystal structures with no P-P pairs bonded (uncollapsed tetragonal, or ucT, state), with one-third of the P-P pairs bonded (one-third collapsed orthorhombic, or tcO, state), or with all P-P pairs bonded (collapsed tetragonal, or cT, state) across the Sr layers. The system can be tuned into its different states by changing temperature, mechanical stress, or chemical composition. Changes in bonding may manifest in changes of macroscopic properties of the material, such as its shape, electrical conductivity, or magnetism. In this work, we show that ${\mathrm{SrNi}}_2{\mathrm{P}}_2$ can be tuned among the three states by changing Cu substitution and temperature. We present temperature-dependent resistance and single-crystal x-ray diffraction results in $\mathrm{Sr}{\left({\mathrm{Ni}}_{1-x}{\mathrm{Cu}}_x\right)}_2{\mathrm{P}}_2$ single-crystals that show that Cu substitution favors the P-P bonding, stabilizing the cT state at ambient pressure. We construct a $T-x$ phase diagram that shows how all of these transition temperatures increase with increasing Cu fraction, $x$. The transition between the tcO state and the cT state exhibits a very large thermal hysteresis, which can be tuned to temperatures close to room temperature. In particular, the properties of Sr(${\mathrm{Ni}}_{0.963}{\mathrm{Cu}}_{0.037}{)}_2{\mathrm{P}}_2$ may make it suitable for applications as a shape-memory material at room temperature.

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• Phase diagrams
• Solid-solid transformations
• Strain
• Crystallography