Determination of the modulated structure of Sr14/11CoO3 through a (3 + 1)-dimensional space description and using non-harmonic ADPs.

Determination of the modulated structure of Sr14/11CoO3 through a (3 + 1)-dimensional space description and using non-harmonic ADPs.
复制标题

通过 (3 1) 维空间描述并使用非谐波 ADP 确定 Sr14/11CoO3 的调制结构。

DOI:
10.1107/s0108768199006485
复制
发表时间:
1999
期刊:
Acta crystallographica. Section B, Structural science
影响因子:
--
通讯作者:
Evain
Evain
中科院分区:
--
文献类型:
--
作者:
Gourdon;Petrı́cek;Dušek;Bezdicka;Durovic;Gyepesova;Evain

文献摘要

被引文献

相似文献

制备了六方钙钛矿结构Sr(x)CoO(3)体系中的一个新相Sr(14/11)CoO(3)(即Sr(14)Co(11)O(33),tetradecastrontiumundecacobalttritriacontaoxide),并利用(3 + 1)维方法从单晶X射线数据解出了它的结构。Sr(14/11)CoO(3)晶体属于三角对称R3;m(00 gamma)0 s超空间群,晶格参数为:a(s)= 9.508(2),c(s)= 2.5343(7)<$,q = 0.63646(11)c(*),V(s)= 198.40(13)<$(3)。由于相称性与不相称性测试没有结论性,该结构被认为是相称的(P32三维空间群),但在(3 + 1)维形式体系内细化为47个参数和1169个独立反射的残差因子R = 0.0351。Crenel函数被用于氧和钴的描述和Gram-Charlier扩展到第三阶的原子位移参数被用于一个Co原子。其结构与Sr(6/5)CoO(3)的结构相似,但沿着[CoO(3)]链的八面体和三角棱镜多面体的顺序不同。一个有趣的功能证明了非谐波膨胀是位移的棱柱Co原子从网站中心,对棱柱矩形面。
Sr(14/11)CoO(3) (i.e. Sr(14)Co(11)O(33), tetradecastrontium undecacobalt tritriacontaoxide), a new phase in the hexagonal perovskite Sr(x)CoO(3) system, has been prepared and its structure solved from single-crystal X-ray data within the (3 + 1)-dimensional formalism. Sr(14/11)CoO(3) crystallizes in the trigonal symmetry, R3;m(00gamma)0s superspace group with the following lattice parameters: a(s) = 9.508 (2), c(s) = 2.5343 (7) Å, q = 0.63646 (11)c(*) and V(s) = 198.40 (13) Å(3). With the commensurate versus incommensurate test not being conclusive, the structure was considered as commensurate (P32 three-dimensional space group), but refined within the (3 + 1)-dimensional formalism to a residual factor R = 0.0351 for 47 parameters and 1169 independent reflections. Crenel functions were used for the oxygen and cobalt description and a Gram-Charlier expansion up to the third order of the atomic displacement parameter was employed for one Co atom. The structure is similar to that of Sr(6/5)CoO(3), but with a different sequence of the octahedra and trigonal prism polyhedra along the [CoO(3)] chains. An interesting feature evidenced by the non-harmonic expansion is the displacement of the prismatic Co atoms from the site center, towards the prism rectangular faces.