Issue |
EPL
Volume 91, Number 5, September 2010
|
|
---|---|---|
Article Number | 56005 | |
Number of page(s) | 6 | |
Section | Condensed Matter: Structural, Mechanical and Thermal Properties | |
DOI | https://doi.org/10.1209/0295-5075/91/56005 | |
Published online | 22 September 2010 |
Interaction between two structural blocks and its correlation with superconductivity in SmFeAsO1-xFx and SmFe1-xMxAsO (M = Co,Ni)
1
Department of Physics, China Jiliang University - Hangzhou 310018, PRC
2
State Key Lab of Silicon Materials, Zhejiang University - Hangzhou 310027, PRC
3
Department of Physics, Zhejiang University - Hangzhou 310027, PRC
Received:
30
April
2010
Accepted:
19
August
2010
Based on a block model, we developed a program to calculate the cohesive energy of the whole cell and the combinative energy between the Fe-As block and the Sm-O block in SmFeAsO1−xFx and SmFe1−xMxAsO (M = Co,Ni). A relationship between the combinative energy and Tc is established, which is similar to the previous reports in cuprate HTSCs to some extent. While the nearly unchanged combinative energy in SmFe1−xMxAsO (M = Co,Ni), no matter whether the electron is supposed to be at the Fe, As site or at the centre of the Fe-As layer, indicates an itinerant character in SmOFeMAs (M = Co,Ni), which is severely different from the local carrier picture in the cuprate HTSCs. We suggest that the relationship can be understood by the charge-transfer models. Our results may shed light on the similarities and differences in understanding the superconductivity of the two important kinds of HTSCs.
PACS: 61.66.Fn – Inorganic compounds / 61.50.Lt – Crystal binding; cohesive energy / 74.70.Dd – Ternary, quaternary, and multinary compounds (including Chevrel phases, borocarbides, etc.)
© EPLA, 2010
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