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相互作用的核壳结构NiO纳米颗粒中的表面自旋玻璃冻结

Surface spin-glass freezing in interacting core-shell NiO nanoparticles.

作者信息

Winkler E, Zysler R D, Vasquez Mansilla M, Fiorani D, Rinaldi D, Vasilakaki M, Trohidou K N

机构信息

Centro Atómico Bariloche, CNEA-CONICET, 8400 S C de Bariloche, RN, Argentina.

出版信息

Nanotechnology. 2008 May 7;19(18):185702. doi: 10.1088/0957-4484/19/18/185702. Epub 2008 Apr 2.

Abstract

Magnetization and AC susceptibility measurements have been performed on ∼3 nm NiO nanoparticles in powder form. The results indicate that the structure of the particles can be considered as consisting of an antiferromagnetically ordered core, with an uncompensated magnetic moment, and a magnetically disordered surface shell. The core magnetic moments block progressively with decreasing temperature, according to the distribution of their anisotropy energy barriers, as shown by a broad maximum of the low field zero-field-cooled magnetization (M(ZFC)) and in the in-phase component χ' of the AC susceptibility, centred at ∼70 K. On the other hand, surface spins thermally fluctuate and freeze in a disordered spin-glass-like state at much lower temperature, as shown by a peak in M(ZFC) (at 17 K, for H = 50 Oe) and in χ'. The temperature of the high temperature χ' peak changes with frequency according to the Arrhenius law; instead, for the low temperature maximum a power law dependence of the relaxation time was found, τ = τ(0)(T(g)/(T(ν)-T(g)))(α), where α = 8, like in spin glasses, τ(0) = 10(-12) s and T(g) = 15.9 K. The low temperature surface spin freezing is accompanied by a strong enhancement of magnetic anisotropy, as shown by the rapid increase of coercivity and high field susceptibility. Monte Carlo simulations for core/shell antiferromagnetic particles, with an antiferromagnetic core and a disordered shell, reproduce the qualitative behaviour of the temperature dependence of the coercivity. Interparticle interactions lead to a shift to a high temperature of the distribution of the core moment blocking temperature and to a reduction of magnetization dynamics.

摘要

已对粉末形式的约3纳米NiO纳米颗粒进行了磁化和交流磁化率测量。结果表明,颗粒结构可被视为由具有未补偿磁矩的反铁磁有序核心和磁无序表面壳层组成。随着温度降低,核心磁矩根据其各向异性能垒的分布逐渐冻结,这表现为低场零场冷却磁化强度(M(ZFC))以及交流磁化率的同相分量χ'出现一个宽泛的最大值,其中心温度约为70K。另一方面,表面自旋在更低温度下热波动并冻结成无序的自旋玻璃态,这表现为M(ZFC)(对于H = 50 Oe时,在17K处)和χ'出现一个峰值。高温χ'峰值的温度根据阿伦尼乌斯定律随频率变化;相反,对于低温最大值,发现弛豫时间具有幂律依赖性,即τ = τ(0)(T(g)/(T(ν)-T(g)))(α),其中α = 8,类似于自旋玻璃,τ(0) = 10^(-12) s且T(g) = 15.9K。低温表面自旋冻结伴随着磁各向异性的强烈增强,这表现为矫顽力和高场磁化率的快速增加。对于具有反铁磁核心和无序壳层的核/壳反铁磁颗粒的蒙特卡罗模拟,再现了矫顽力温度依赖性的定性行为。颗粒间相互作用导致核心磁矩阻塞温度分布向高温偏移,并使磁化动力学降低。

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