Köseoğlu Yüksel, Yildiz Hayrettin, Yilgin Resul
Fatih University, Department of Physics, Buyukcekmece, 34500 Istanbul, Turkey.
J Nanosci Nanotechnol. 2012 Mar;12(3):2261-9. doi: 10.1166/jnn.2012.5718.
Superparamagnetic nanoparticles of zinc ferrite (ZnFe2O4) were produced by a microwave induced combustion synthesis method. XRD, FT-IR, SEM, VSM and ESR were used for the structural, morphological, and magnetic investigation of the product, respectively. Average particle size of the nanoparticles was estimated by the Schérrer equation using the full-width at half maximum (FWHM) of the most intense XRD peak and found as 41 nm. Magnetization measurements have shown that the samples have a blocking temperature of 72 K which indicates a superparamagnetic behavior. Superparamagnetic resonance (SPR) spectra at room temperature show a broad line with a Landé g-factor, g(eff) approximately 2. We used a theoretical formalism based on a distribution of diameters of the nanoparticles following lognormal proposed by Berger et al. The nanoparticles behave as single magnetic domains with random orientations of magnetic moments which are subject to thermal fluctuations. A Landau-Lifshitz line shape function presents adequate results which are in good agreement with the experimental ones. At high temperatures, the SPR line shape is governed by the core anisotropy and the thermal fluctuations. By decreasing the temperature, the magnetic susceptibility of shell spins increases. As a result of this, the surface spins produce an effective field on the core leading to a decrease of resonance field, B(r). Also, the effective anisotropy increases as the shell spins begin to order. So, the results are interpreted by a simple model, in which each single-domain nanoparticle is considered as a core-shell system, with magneto-crystalline anisotropy on the core and surface anisotropy on the shell.
采用微波诱导燃烧合成法制备了铁酸锌(ZnFe₂O₄)超顺磁性纳米颗粒。分别利用X射线衍射(XRD)、傅里叶变换红外光谱(FT-IR)、扫描电子显微镜(SEM)、振动样品磁强计(VSM)和电子自旋共振(ESR)对产物进行结构、形态和磁性研究。利用Schérrer方程,通过最强烈XRD峰的半高宽(FWHM)估算纳米颗粒的平均粒径,结果为41 nm。磁化测量表明,样品的阻塞温度为72 K,表明具有超顺磁性行为。室温下的超顺磁共振(SPR)光谱显示出一条宽线,朗德g因子g(eff)约为2。我们使用了一种基于Berger等人提出的对数正态分布的纳米颗粒直径分布的理论形式。纳米颗粒表现为单磁畴,磁矩具有随机取向,且受到热涨落的影响。Landau-Lifshitz线形函数给出了与实验结果吻合良好的充分结果。在高温下,SPR线形由核心各向异性和热涨落决定。随着温度降低,壳层自旋的磁化率增加。由此,表面自旋在核心上产生一个有效场,导致共振场B(r)减小。此外,随着壳层自旋开始有序排列,有效各向异性增加。因此,结果可以用一个简单模型来解释,其中每个单畴纳米颗粒被视为一个核壳系统,核心具有磁晶各向异性,壳层具有表面各向异性。