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氧化学计量比对 Sr2CoIrO(6-δ) 的相稳定性、结构和磁性能的作用。

The role of oxygen stoichiometry on phase stability, structure, and magnetic properties of Sr2CoIrO(6-δ).

机构信息

Institute for Complex Materials, IFW Dresden, Helmholtzstrasse 20, D-01069 Dresden, Germany.

出版信息

Inorg Chem. 2010 Nov 15;49(22):10348-56. doi: 10.1021/ic100973p. Epub 2010 Oct 21.

DOI:10.1021/ic100973p
PMID:20964307
Abstract

The phase stability, crystal structure, and magnetic properties of perovskite-like nonstoichiometric Sr(2)CoIrO(6-δ) were studied. Oxygen deficiency can be well controlled and reversibly varied up to δ = 0.33. A single phase exists at least for partial oxygen pressures between 10(-5) and 1 bar at 1273 K, followed by phase decomposition at higher temperature with the elimination of metallic Ir and the formation of a new phase with approximately Sr(3)CoIrO(6) composition crystallizing in K(4)CdCl(6) structure type. The structural features of Sr(2)CoIrO(6-δ) are dependent on both temperature and oxygen content and were determined by synchrotron and neutron powder diffraction. Both the increasing amount of oxygen vacancies at constant temperature and increasing temperature at constant oxygen content result in the same higher crystal symmetry of Sr(2)CoIrO(6-δ): (1) The oxygen-stoichiometric phase Sr(2)CoIrO(6.00) is monoclinic (I2/m or P2(1)/n) at room temperature but cubic (Fm-3m) for Sr(2)CoIrO(5.67). (2) A sequence of phase transitions [Formula: see text] was observed for Sr(2)CoIrO(6.00) in air. All Sr(2)CoIrO(6-δ) compositions show weak ferromagnetism at low temperature with a canted but predominantly antiferromagnetic ground state. The magnetic ordering temperature decreases monotonously with increasing oxygen deficiency, while pronounced extrema are observed for the paramagnetic moment and the Curie-Weiss temperature at an oxygen deficiency δ ≈ 0.10, which corresponds to the P2(1)/n ↔ I2/m phase transformation.

摘要

钙钛矿型非化学计量比 Sr(2)CoIrO(6-δ) 的相稳定性、晶体结构和磁性能进行了研究。氧空位可以很好地控制并在 δ = 0.33 时可逆变化。在 1273 K 时,至少在 10(-5) 和 1 巴之间的部分氧分压下存在单相,随后在较高温度下发生相分解,去除金属 Ir 并形成具有约 Sr(3)CoIrO(6)组成的新相,该新相在 K(4)CdCl(6)结构类型中结晶。Sr(2)CoIrO(6-δ) 的结构特征取决于温度和氧含量,并通过同步加速器和中子粉末衍射确定。在恒温下增加氧空位的数量和在恒温下增加温度都会导致 Sr(2)CoIrO(6-δ)的更高晶体对称性:(1) 氧化学计量相 Sr(2)CoIrO(6.00)在室温下为单斜晶系(I2/m 或 P2(1)/n),但在 Sr(2)CoIrO(5.67)时为立方晶系(Fm-3m)。(2) 在空气中观察到 Sr(2)CoIrO(6.00)的一系列相变[Formula: see text]。所有 Sr(2)CoIrO(6-δ) 组成物在低温下表现出弱铁磁性,具有倾斜但主要反铁磁基态。随着氧空位的增加,磁有序温度单调下降,而在氧空位 δ ≈ 0.10 时,顺磁矩和居里-外斯温度观察到明显的极值,这对应于 P2(1)/n ↔ I2/m 相变。

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