Abstract

In this study, we succeeded in synthesizing new antiperovskite phosphides MMPd3_3P (MM = Ca, Sr, Ba) and discovered the appearance of a superconducting phase (0.17 ≤\leq xx ≤\leq 0.55) in a solid solution (Ca1−x_{1-x}Srx_x)Pd3_3P. Three perovskite-related crystal structures were identified in (Ca1−x_{1-x}Srx_x)Pd3_3P and a phase diagram was built on the basis of experimental results. The first phase transition from centrosymmetric (PnmaPnma) to non-centrosymmetric orthorhombic (AbaAba2) occurred in CaPd3_3P near room temperature. The phase transition temperature decreased as Ca2+^{2+} was replaced with a larger-sized isovalent Sr2+^{2+}. Bulk superconductivity at a critical temperature (TTc_c) of approximately 3.5 K was observed in a range of xx = 0.17 - 0.55; this was associated with the centrosymmetric orthorhombic phase. Thereafter, a non-centrosymmetric tetragonal phase (II41mdmd) remained stable for 0.6 ≤\leq xx ≤\leq 1.0, and superconductivity was significantly suppressed as samples with xx = 0.75 and 1.0 showed (TTc_c) values as low as 0.32 K and 57 mK, respectively. For further substitution with a larger-sized isovalent Ba2+^{2+}, namely (Sr1−y_{1-y}Bay_y)Pd3_3P, the tetragonal phase continued throughout the composition range. BaPd3_3P no longer showed superconductivity down to 20 mK. Since the inversion symmetry of structure and superconductivity can be precisely controlled in (Ca1−x_{1-x}Srx_x)Pd3_3P, this material may offer a unique opportunity to study the relationship between inversion symmetry and superconductivity.

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