基于组分Ca2Pr2Cu5O10三元固溶区的范围和晶体结构

宋功保 韩苍穹 梁敬魁 饶光辉

宋功保, 韩苍穹, 梁敬魁, 饶光辉. 基于组分Ca2Pr2Cu5O10三元固溶区的范围和晶体结构[J]. 高压物理学报, 2004, 18(1): 27-35 . doi: 10.11858/gywlxb.2004.01.006
引用本文: 宋功保, 韩苍穹, 梁敬魁, 饶光辉. 基于组分Ca2Pr2Cu5O10三元固溶区的范围和晶体结构[J]. 高压物理学报, 2004, 18(1): 27-35 . doi: 10.11858/gywlxb.2004.01.006
SONG Gong-Bao, HAN Cang-Qiong, LIANG Jing-Kui, RAO Guang-Hui. The Extent and Crystal Structure of the Solid Solution Based on Ca2Pr2Cu5O10[J]. Chinese Journal of High Pressure Physics, 2004, 18(1): 27-35 . doi: 10.11858/gywlxb.2004.01.006
Citation: SONG Gong-Bao, HAN Cang-Qiong, LIANG Jing-Kui, RAO Guang-Hui. The Extent and Crystal Structure of the Solid Solution Based on Ca2Pr2Cu5O10[J]. Chinese Journal of High Pressure Physics, 2004, 18(1): 27-35 . doi: 10.11858/gywlxb.2004.01.006

基于组分Ca2Pr2Cu5O10三元固溶区的范围和晶体结构

doi: 10.11858/gywlxb.2004.01.006
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    通讯作者:

    宋功保

The Extent and Crystal Structure of the Solid Solution Based on Ca2Pr2Cu5O10

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    Corresponding author: SONG Gong-Bao
  • 摘要: 利用X射线衍射分析和Rietveld结构精修方法研究了基于组分Ca2Pr2Cu5O10三元固溶区的范围和晶体结构。根据X射线分析结果和相消失法,为了保持Ca2+xPr2-xCu5O10结构单位晶胞中恒定的氧含量和电价平衡,基于组分Ca2Pr2Cu5O10的三元固溶区的范围可确定为:在Ca2+xPr2-xCu5O10固溶区的富Ca区(Ca/Pr1),其表达式仍可以表示为一般的化学计量式Ca2+xPr2-xCu5O10(x=0.4, 0.2, 0);在富Pr区(Ca/Pr1),其表达式为Ca1.7Pr2.2Cu5O10、Ca1.4Pr2.4Cu5O10,即:Ca2+xPr2-xCu5O10固溶区范围从Ca2.4Pr1.6Cu5O10至Ca1.4Pr2.4Cu5O10。研究表明:基于组分Ca2Pr2Cu5O10的三元固溶体晶体结构可以看作是正交晶系NaCuO2型亚晶胞的无公度相;Ca2.4Pr1.6Cu5O10亚晶胞的点阵常数为a0=0.282 46(7) nm,b0=0.636 93(1) nm,c0=1.067 94(1) nm;其正交超结构的点阵常数为a=5a0,b=b0,c=5c0。Ca2.4Pr1.6Cu5O10的结构也可以用单斜超晶胞来表述,该单斜超晶胞的空间群为P21/c,Z=4,a=5a0,b=b0,c=c0/sin ,=104.79或136.60,V=5a0b0c0。在基于组分Ca2Pr2Cu5O10的三元固溶体晶体结构中,Ca和Pr之间在一定范围内是可以相互替代的,而且它们在结构中的占位是无序的。

     

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出版历程
  • 收稿日期:  2003-05-24
  • 修回日期:  2003-09-22
  • 刊出日期:  2004-03-05

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