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通过 Jahn-Teller 畸变对 Nd₂GaMnO₆ 和 La₂GaMnO₆ 中磁有序的控制

Control of magnetic ordering by Jahn--Teller distortions in Nd(2)GaMnO(6) and La(2)GaMnO(6).

作者信息

Cussen E J, Rosseinsky M J, Battle P D, Burley J C, Spring L E, Vente J F, Blundell S J, Coldea A I, Singleton J

机构信息

Department of Chemistry, University of Liverpool, Liverpool L69 7ZD, UK.

出版信息

J Am Chem Soc. 2001 Feb 14;123(6):1111-22. doi: 10.1021/ja003139i.

Abstract

The substitution of Ga(3+) into the Jahn--Teller distorted, antiferromagnetic perovskites LaMnO(3) and NdMnO(3) strongly affects both the crystal structures and resulting magnetic ordering. In both compounds the Ga(3+) and Mn(3+) cations are disordered over the six coordinate sites. La(2)GaMnO(6) is a ferromagnetic insulator (T(c) = 70 K); a moment per Mn cation of 2.08(5) mu(B) has been determined by neutron powder diffraction at 5 K. Bond length and displacement parameter data suggest Jahn--Teller distortions which are both coherent and incoherent with the Pnma space group symmetry of the perovskite structure (a = 5.51122(4) A, b = 7.80515(6) A, c = 5.52947(4) A) at room temperature. The coherent distortion is strongly suppressed in comparison with the parent LaMnO(3) phase, but the displacement ellipsoids suggest that incoherent distortions are significant and arise from local Jahn--Teller distortions. The preparation of the new phase Nd(2)GaMnO(6) has been found to depend on sample cooling rates, with detailed characterization necessary to ensure phase separation has been avoided. This compound also adopts the GdFeO(3)-type orthorhombically distorted perovskite structure (space group Pnma, a = 5.64876(1) A, b = 7.65212(2) A, c = 5.41943(1) A at room temperature). However, the B site substitution has a totally different effect on the Jahn--Teller distortion at the Mn(3+) centers. This phase exhibits a Q(2) mode Jahn--Teller distortion similar to that observed in LaMnO(3), although reduced in magnitude as a result of the introduction of Ga(3+) onto the B site. There is no evidence of a dynamic Jahn-Teller distortion. At 5 K a ferromagnetically ordered Nd(3+) moment of 1.06(6) mu(B) is aligned along the y-axis and a moment of 2.8(1) mu(B) per Mn(3+) is ordered in the xy plane making an angle of 29(2) degrees with the y-axis. The Mn(3+) moments couple ferromagnetically in the xz plane. However, along the y-axis the moments couple ferromagnetically while the x components are coupled antiferromagnetically. This results in a canted antiferromagnetic arrangement in which the dominant exchange is ferromagnetic. Nd(2)GaMnO(6) is paramagnetic above 40(5) K, with a paramagnetic moment and Weiss constant of 6.70(2) mu(B) and 45.9(4) K, respectively. An ordered moment of 6.08(3) mu(B) per Nd(2)GaMnO(6) formula unit was measured by magnetometry at 5 K in an applied magnetic field of 5 T.

摘要

将Ga(3+) 取代 Jahn-Teller 畸变的反铁磁钙钛矿 LaMnO(3) 和 NdMnO(3) 中的离子,会强烈影响晶体结构以及由此产生的磁有序性。在这两种化合物中,Ga(3+) 和 Mn(3+) 阳离子在六个配位位点上无序分布。La(2)GaMnO(6) 是一种铁磁绝缘体(居里温度 T(c) = 70 K);通过 5 K 下的中子粉末衍射确定每个 Mn 阳离子的磁矩为 2.08(5) μB。键长和位移参数数据表明,Jahn-Teller 畸变在室温下与钙钛矿结构(a = 5.51122(4) Å,b = 7.80515(6) Å,c = 5.52947(4) Å)的 Pnma 空间群对称性既有相干的,也有非相干的。与母体 LaMnO(3) 相相比,相干畸变受到强烈抑制,但位移椭球体表明非相干畸变很显著,且源于局部 Jahn-Teller 畸变。已发现新相 Nd(2)GaMnO(6) 的制备取决于样品冷却速率,需要进行详细表征以确保避免相分离。该化合物也采用 GdFeO(3) 型正交畸变钙钛矿结构(空间群 Pnma,室温下 a = 5.64876(1) Å,b = 7.65212(2) Å,c = 5.41943(1) Å)。然而,B 位取代对 Mn(3+) 中心的 Jahn-Teller 畸变有完全不同的影响。该相表现出与 LaMnO(3) 中观察到的类似的 Q(2) 模式 Jahn-Teller 畸变,尽管由于在 B 位引入 Ga(3+) 而使其幅度减小。没有动态 Jahn-Teller 畸变的证据。在 5 K 时,1.06(6) μB 的铁磁有序 Nd(3+) 磁矩沿 y 轴排列,每个 Mn(3+) 在 xy 平面内有 2.8(1) μB 的磁矩,与 y 轴成 29(2) 度角。Mn(3+) 磁矩在 xz 平面内铁磁耦合。然而,沿 y 轴磁矩铁磁耦合,而 x 分量反铁磁耦合。这导致一种倾斜反铁磁排列,其中主要的交换是铁磁的。Nd(2)GaMnO(6) 在 40(5) K 以上是顺磁性的,顺磁矩和魏斯常数分别为 6.70(2) μB 和 45.9(4) K。在 5 T 的外加磁场中,通过磁强计测量得到每个 Nd(2)GaMnO(6) 化学式单元在 5 K 时的有序磁矩为 6.08(3) μB。

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