Mn(PtPd)P: Isovalent Tuning of Mn Sublattice Magnetic Order
arXiv:2211.01818 · doi:10.1103/PhysRevB.107.134429
Abstract
We report the growth and characterization of MnPdP, a ferromagnet with T 295 K, and conduct a substitutional study with its antiferromagnetic analogue MnPtP. We grow single crystals of MnPdP and Mn(PtPd)P by adding Mn into (PtPd)-P based melts. All compounds in the family adopt the layered anti-CeCoIn structure with space group P4/mmm, and EDS and XRD results indicate that MnPtP and MnPdP form a solid solution. Based on magnetization and resistance data, we construct a T-x phase diagram for Mn(PtPd)P and demonstrate the antiferromagnetic order found in MnPtP is extraordinarily sensitive to Pd substitution. At low Pd fractions (x 0.010), the single antiferromagnetic transition in pure MnPtP splits into a higher temperature ferromagnetic transition followed on cooling by a lower temperature ferromagnetic to antiferromagnetic transition and then by a re-entrant antiferromagnetic to ferromagnetic transition at lower temperatures. The antiferromagnetic region makes up a bubble that persists to x 0.009 for T 150 K, with all samples x 0.009 recovering their initial ferromagnetic state with further cooling to base temperature. Over the same low x range we find a non-monotonic change in the room temperature unit cell volume, further suggesting that pure MnPtP is close to an instability. Once x 0.010, Mn(PtPd)P undergoes a single ferromagnetic transition. The Curie temperature increases rapidly with x, rising from T 197 K at x = 0.013 to a maximum of T 312 K for x 0.62, and then falls back to T 295 K for pure MnPdP (x = 1). Given that Pt and Pd are isoelectronic, this work raises questions as to the origin of the extreme sensitivity of the magnetic ground state in MnPtP upon introducing Pd.
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