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单相CoO纳米颗粒中的尺寸诱导交换偏置

Size-induced exchange bias in single-phase CoO nanoparticles.

作者信息

Sharma Vikash, Pal Sudip, Sharma Divya, Shukla Dinesh Kumar, Chaudhary Ram Janay, Okram Gunadhor Singh

机构信息

UGC-DAE Consortium for Scientific Research University campus, Khandwa road, Indore-452001, Madhya Pradesh, India.

Govt. Girls PG College, Ujjain-456010, MP, India.

出版信息

Nanotechnology. 2024 Apr 18;35(27). doi: 10.1088/1361-6528/ad3256.

Abstract

The tuning of exchange bias (EB) in nanoparticles has garnered significant attention due to its diverse range of applications. Here, we demonstrate EB in single-phase CoO nanoparticles, where two magnetic phases naturally emerge as the crystallite size decreases from 34.6 ± 0.8 to 10.8 ± 0.9 nm. The Néel temperature () associated with antiferromagnetic ordering decreases monotonically with the reduction in crystallite size, highlighting the significant influence of size effects. The 34.6 nm nanoparticles exhibit magnetization irreversibility between zero-field cooled (ZFC) and field-cooled (FC) states below. With further reduction in size this irreversibility appears well above, resulting in the absence of true paramagnetic regime which indicates the occurnace of an additional magnetic phase. The frequency-dependent ac-susceptibility in 10.8 nm nanoparticles suggests slow dynamics of disordered surface spins above, coinciding with the establishment of long-range order in the core. The thermoremanent magnetization (TRM) and iso-thermoremanent magnetization (IRM) curves suggest a core-shell structure: the core is antiferromagnetic, and the shell consists of disordered surface spins causing ferromagnetic interaction. Hence, the EB in these CoO nanoparticles results from the exchange coupling between an antiferromagnetic core and a disordered shell that exhibits unconventional surface spin characteristics.

摘要

由于其广泛的应用范围,纳米颗粒中交换偏置(EB)的调控已引起了广泛关注。在此,我们展示了单相CoO纳米颗粒中的EB,随着微晶尺寸从34.6±0.8纳米减小到10.8±0.9纳米,两个磁相自然出现。与反铁磁有序相关的奈尔温度()随着微晶尺寸的减小而单调降低,突出了尺寸效应的显著影响。34.6纳米的纳米颗粒在低于零场冷却(ZFC)和场冷却(FC)状态之间表现出磁化不可逆性。随着尺寸的进一步减小,这种不可逆性出现在更高温度下,导致不存在真正的顺磁态,这表明出现了额外的磁相。10.8纳米纳米颗粒中频率依赖的交流磁化率表明,在上述温度以上无序表面自旋的动力学缓慢,这与核心中长程有序的建立相吻合。热剩磁(TRM)和等温剩磁(IRM)曲线表明存在核壳结构:核心是反铁磁的,壳层由导致铁磁相互作用的无序表面自旋组成。因此,这些CoO纳米颗粒中的EB源于反铁磁核心与表现出非常规表面自旋特性的无序壳层之间的交换耦合。

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