Abstract
Cubic SrCoO3 with an intermediate spin state can only be stabilized by high pressure and high temperature (HPHT) treatment. It is metallic and ferromagnetic with the highest Curie temperature of the transition-metal perovskites. The chemical substitution by Ca on Sr sites would normally lower crystal symmetry from cubic to orthorhombic as seen in the perovskite family of CaMO3 (M=M4+ of transition metals, Ge4+, Sn4+, and Zr4+) at room temperature. This structural change narrows the bandwidth, so as to further enhance the Curie temperature as the crossover to the localized electronic state is approached. We report a successful synthesis of the perovskite CaCoO3 with a HPHT treatment. Surprisingly, CaCoO3 crystallizes in a simple cubic structure that remains stable down to 20 K, the lowest temperature in the structural study. The new perovskite has been thoroughly characterized by a suite of measurements including transport, magnetization, specific heat, thermal conductivity, and thermoelectric power. Metallic CaCoO3 undergoes two successive magnetic transitions at 86 K and 54 K as temperature decreases. The magnetization at 5 K is compatible with the intermediate spin state t4e1 of Co4+ at the octahedral site. The thermal expansion of the Co-O bond length indicates that the population of high spin state t3e2 increases for T>100K. The shortest Co-O bond length in cubic CaCoO3 is responsible for delocalizing electrons in the π∗-band and itinerant-electron ferromagnetism at T<54K. A comprehensive comparison between SrCoO3 and CaCoO3 and the justification of their physical properties by first-principles calculation have also been made in this report. Partially filled π∗ and σ∗ bands would make CaCoO3 suitable to study the Hund's coupling effect in a metal.
Original language | English |
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Article number | 024406 |
Journal | Physical Review Materials |
Volume | 1 |
Issue number | 2 |
DOIs | |
State | Published - Jul 17 2017 |
Funding
The authors are grateful to Q. F. Zhang, Z. G. Sheng, and J. Q. Yan for enlightening discussion and to J. B. Goodenough for reviewing and commenting on the manuscript. This work was supported by the 973 Project of the Ministry of Science and Technology of China (Grant No. 2014CB921500), the Strategic Priority Research Program of the Chinese Academy of Sciences (Grant No. XDB07030300), and the National Natural Science Foundation of China (Grant No. 11574378). J.S.Z. was supported by DOD-ARMY (W911NF-16-1-0559). M.A.M. acknowledges support from the US Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division.
Funders | Funder number |
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DOD-ARMY | W911NF-16-1-0559 |
U.S. Department of Energy | |
Office of Science | |
Basic Energy Sciences | |
Division of Materials Sciences and Engineering | |
National Natural Science Foundation of China | 11574378 |
Chinese Academy of Sciences | XDB07030300 |
Ministry of Science and Technology of the People's Republic of China | 2014CB921500 |
National Key Research and Development Program of China |