The role played by Ni impurities in destroying the superconducting state of La2-xSrxCuO4 is still unclear. This is partly due to the lack of clear experimental evidence on the effect of Ni substitution upon the atomic and electronic structure of this cuprate. To provide this information, we performed Ni K-edge polarized XAFS measurements on oriented powder. A special magnetic alignment geometry allowed us to measure pure ĉ and âb-polarized XAFS in identical experimental conditions. We found that the NiO6 octahedra are contracted along the ĉ-axis by 0.16(Å) relative to the CuO6 octahedra in La1.85Sr0.15CuO4, dragging La atoms and causing the observed macroscopic ĉ-axis contraction. This contraction reflects the non-Jahn-Teller 3d8 state of Ni in this compound (similar to that in La2NiO4) and indicates that Ni does not "trap" hole carriers but rather, probably, "repels" them. We suggest that this repulsion is the mechanism behind Tc suppression.
D. Haskel et al., "Why does Ni suppress superconductivity in La₁.₈₅Sr₀.₁₅Cu1-yNiyO₄?," Journal of Synchrotron Radiation, vol. 6, no. 3, pp. 758 - 760, International Union of Crystallography, May 1999.
The definitive version is available at https://doi.org/10.1107/S090904959900148X
Materials Science and Engineering
Keywords and Phrases
Jahn-Teller; Nickel doping; Superconductivity
International Standard Serial Number (ISSN)
Article - Journal
© 1999 International Union of Crystallography, All rights reserved.
01 May 1999