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SrCuO(一种不含氧化铜平面的95K铜酸盐超导体)的局部结构

Local structure of SrCuO, a 95 K cuprate superconductor without CuO planes.

作者信息

Conradson Steven D, Geballe Theodore H, Jin Changqing, Cao Lipeng, Baldinozzi Gianguido, Jiang Jack M, Latimer Matthew J, Mueller Oliver

机构信息

Department of Complex Matter, Jozef Stefan Institute, 1000 Ljubljana, Slovenia.

Department of Chemistry, Washington State University, Pullman, WA 99164.

出版信息

Proc Natl Acad Sci U S A. 2020 Mar 3;117(9):4565-4570. doi: 10.1073/pnas.1918890117. Epub 2020 Feb 14.

Abstract

The local structure of the highly "overdoped" 95 K superconductor SrCuO determined by Cu K X-ray absorption fine structure (XAFS) at 62 K in magnetically oriented samples shows that 1) the magnetization is perpendicular to the axis; 2) at these levels of precision the Cu sublattice is tetragonal in agreement with the crystal structure; the O sublattice has 3) continuous -Cu-O- chains that orient perpendicular to an applied magnetic field; 4) approximately half-filled -Cu-O- chains that orient parallel to this field; 5) a substantial number of apical O vacancies; 6) O ions at some apical positions with expanded Cu-O distances; and 7) interstitial positions that imply highly displaced Sr ions. These results contradict the universally accepted features of cuprates that require intact CuO planes, magnetization along the axis, and a termination of the superconductivity when the excess charge on the CuO Cu ions exceeds 0.27. These radical differences in charge and structure demonstrate that this compound constitutes a separate class of Cu-O-based superconductors in which the superconductivity originates in a different, more complicated structural unit than CuO planes while retaining exceptionally high transition temperatures.

摘要

通过对磁取向样品在62K下进行Cu K X射线吸收精细结构(XAFS)测定得到的高度“过掺杂”的95K超导体SrCuO的局部结构表明:1)磁化方向垂直于 轴;2)在这些精度水平下,Cu亚晶格为四方结构,与晶体结构一致;O亚晶格有3)垂直于外加磁场取向的连续-Cu-O-链;4)大约一半填充的平行于该磁场取向的-Cu-O-链;5)大量的顶端O空位;6)一些顶端位置的O离子,其Cu-O距离增大;7)间隙位置表明Sr离子高度位移。这些结果与铜酸盐普遍接受的特征相矛盾,铜酸盐要求完整的CuO平面、沿 轴的磁化,以及当CuO Cu离子上的过量电荷超过0.27时超导性终止。这些电荷和结构上的根本差异表明,该化合物构成了一类单独的基于Cu-O的超导体,其中超导性起源于与CuO平面不同的、更复杂的结构单元,同时保持了异常高的转变温度。

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