论文标题

在Antiperovskite磷化物CAPD $ _3 $ P中引起的结构相变和超导率

Structural phase transitions and superconductivity induced in antiperovskite phosphide CaPd$_3$P

论文作者

Iyo, Akira, Fujihisa, Hiroshi, Gotoh, Yoshito, Ishida, Shigeyuki, Ninomiya, Hiroki, Yoshida, Yoshiyuki, Eisaki, Hiroshi, Hirose, Hishiro T., Terashima, Taichi, Kawashima, Kenji

论文摘要

在这项研究中,我们成功地合成了新的Antiperovskite磷酸​​盐$ m $ pd $ _3 $ _3 $ p($ m $ = ca,sr,ba),并发现了超导阶段的外观(0.17 $ \ leq $ $ $ $ x $ x $ $ $ \ $ \ leq $ 0.55)在(CA $ _ {1-X} $ SR $ _X $)PD $ _3 $ P中确定了三个与钙钛矿相关的晶体结构,并根据实验结果构建了相位图。从中心对称($ PNMA $)到非中心对称原晶($ aba $ 2)的第一阶段过渡发生在CAPD $ _3 $ P附近的室温。当Ca $^{2+} $被大尺寸的Isovalent SR $^{2+} $取代时,相变温度降低。在$ x $ = 0.17-0.55的范围内观察到在临界温度($ t $$ _ c $)下的散装超导率;这与中心对称的正交相有关。此后,一个非中心的四方阶段($ i $ 41 $ md $)仍然保持稳定,以0.6 $ \ leq $ $ $ $ x $ x $ $ \ $ \ leq $ 1.0 $ 1.0,超导性被显着抑制为样品,$ x $ = 0.75和1.0显示($ t $ t $ _ c $ _c $ _ c $ _ C $),如0.32 K和0.32 K和57 Mk,并且相差57 MK,并且要用较大尺寸的Isovalent ba $^{2+} $替换,即(sr $ _ {1-y} $ ba $ _y $)pd $ _3 $ p,在整个构图范围内,四方阶段持续。 bapd $ _3 $ p不再显示超导率降至20 mk。由于可以在(CA $ _ {1-X} $ sr $ _X $)PD $ _3 $ P中精确控制结构和超导性的反转对称性,因此该材料可能会提供一个独特的机会来研究反转对称性和超导率之间的关系。

In this study, we succeeded in synthesizing new antiperovskite phosphides $M$Pd$_3$P ($M$ = Ca, Sr, Ba) and discovered the appearance of a superconducting phase (0.17 $\leq$ $x$ $\leq$ 0.55) in a solid solution (Ca$_{1-x}$Sr$_x$)Pd$_3$P. Three perovskite-related crystal structures were identified in (Ca$_{1-x}$Sr$_x$)Pd$_3$P and a phase diagram was built on the basis of experimental results. The first phase transition from centrosymmetric ($Pnma$) to non-centrosymmetric orthorhombic ($Aba$2) occurred in CaPd$_3$P near room temperature. The phase transition temperature decreased as Ca$^{2+}$ was replaced with a larger-sized isovalent Sr$^{2+}$. Bulk superconductivity at a critical temperature ($T$$_c$) of approximately 3.5 K was observed in a range of $x$ = 0.17 - 0.55; this was associated with the centrosymmetric orthorhombic phase. Thereafter, a non-centrosymmetric tetragonal phase ($I$41$md$) remained stable for 0.6 $\leq$ $x$ $\leq$ 1.0, and superconductivity was significantly suppressed as samples with $x$ = 0.75 and 1.0 showed ($T$$_c$) values as low as 0.32 K and 57 mK, respectively. For further substitution with a larger-sized isovalent Ba$^{2+}$, namely (Sr$_{1-y}$Ba$_y$)Pd$_3$P, the tetragonal phase continued throughout the composition range. BaPd$_3$P no longer showed superconductivity down to 20 mK. Since the inversion symmetry of structure and superconductivity can be precisely controlled in (Ca$_{1-x}$Sr$_x$)Pd$_3$P, this material may offer a unique opportunity to study the relationship between inversion symmetry and superconductivity.

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