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Local structure of Sr2CuO3.3, a 95 K cuprate superconductor without CuO2 planes
Steven D Conradson1,2, Theodore H Geballe3,4,5, Changqing Jin6,7,8
1Department of Complex Matter, Jozef Stefan Institute, 1000 Ljubljana, Slovenia.
This study reveals novel structural features in the Sr2CuO3.3 superconductor, challenging existing models of cuprate superconductivity. The findings suggest a new class of superconductors with unique charge and structural properties.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Superconductivity
Background:
- Cuprate superconductors typically exhibit intact CuO2 planes and magnetization along the c-axis.
- Superconductivity in cuprates is thought to terminate when excess charge exceeds 0.27.
- The local structure of overdoped Sr2CuO3.3 has not been fully elucidated.
Purpose of the Study:
- To determine the local structure of the superconductor Sr2CuO3.3 using X-ray absorption fine structure.
- To investigate the relationship between structure, charge, and superconductivity in this overdoped cuprate.
- To challenge established models of cuprate superconductivity.
Main Methods:
- Cu K X-ray absorption fine structure (XAFS) spectroscopy.
- Magnetically oriented sample preparation.
- Analysis of local atomic arrangements and bonding.
Main Results:
- Magnetization is perpendicular to the c-axis, contrary to typical cuprates.
- Cu sublattice is tetragonal; oxygen sublattice features continuous and half-filled Cu-O chains.
- Significant apical oxygen vacancies and displaced Sr ions were observed, challenging standard CuO2 plane models.
Conclusions:
- Sr2CuO3.3 exhibits a unique structure and charge distribution, classifying it as a new type of Cu-O-based superconductor.
- Superconductivity in this material likely originates from a more complex structural unit than CuO2 planes.
- The findings necessitate a revision of the universally accepted features of cuprate superconductors.
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