Spin-state transition, magnetism and local crystal structure in Eu 1-xCaxCoO3-δ

Alexander N. Vasiliev*, Tatyana M. Vasilchikova, Olga S. Volkova, Anton A. Kamenev, Andrey R. Kaul, Tatyana G. Kuzmova, Dmitry M. Tsymbarenko, Kirill A. Lomachenko, Alexander V. Soldatov, Sergey V. Streltsov, Jiunn-Yuan Lin, Cheng Nan Kao, Jin Ming Chen, Mahmoud Abdel-Hafiez, Anja Wolter, Rüdiger Klingeler

*Corresponding author for this work

Research output: Contribution to journalArticlepeer-review

2 Scopus citations

Abstract

The doping series Eu1-xCaxCoO3-δ provides a rather peculiar way to study the spin-state transitions in cobalt-based complex oxides since partial substitution of Eu3+ ions by Ca2+ ions does not increase the mean valence of cobalt but is accompanied by appearance of oxygen vacancies in the ratio δ ~ x/2. In the parent compound EuCoO3, the low spin (LS)-intermediate spin (IS) or high spin (HS) transition takes place at temperatures so high that the chemical decomposition prevents its direct observation. The substitution of Eu 3+ by Ca2+ shifts the spin state transition to lower temperatures and the associated energy gap Δ in octahedrally-coordinated Co3+ ions changes from 1940K in EuCoO3 to 1540K in Eu 0.9Ca0.1CoO2.95 and 1050K in Eu 0.8Ca0.2CoO2.9. Besides, each O2- vacancy reduces the local coordination of two neighboring Co3+ ions from octahedral to pyramidal thereby locally creating magnetically active sites which couple to dimers. These dimers form another gapped magnetic system with a very different energy scale, Ddim ~ 3 K, on the background of the intrinsically non-magnetic lattice of octahedrally-coordinated low-spin Co 3+ ions.

Original languageEnglish
Article number044714
JournalJournal of the Physical Society of Japan
Volume82
Issue number4
DOIs
StatePublished - 1 Apr 2013

Keywords

  • Cobaltites
  • Local crystal structure
  • Magnetic susceptibility
  • Specific heat
  • Spin state transitions
  • XANES

Fingerprint

Dive into the research topics of 'Spin-state transition, magnetism and local crystal structure in Eu 1-xCaxCoO3-δ'. Together they form a unique fingerprint.

Cite this