Bibani Malek, Breitwieser Romain, Aubert Alex, Loyau Vincent, Mercone Silvana, Ammar Souad, Mammeri Fayna
Université Paris Diderot, Sorbonne Paris Cité, ITODYS UMR CNRS 7086.
ENS Paris Saclay, SATIE UMR CNRS 8029, 61 Avenue du Président Wilson, 94235 Cachan Cedex, France.
Beilstein J Nanotechnol. 2019 Jun 4;10:1166-1176. doi: 10.3762/bjnano.10.116. eCollection 2019.
In extrinsically magnetoelectric materials made of two components, the direct magnetoelectric coupling arises from a mechanical strain transmission at the interface due to the shape change of the magnetostrictive component under an external magnetic field. Here, the size of the interface between the two components plays a crucial role. Therefore, the development of nanomaterials exhibiting large surface-to-volume ratios can help to respond to such a requirement. However, the magnetic nanoparticles (NPs) must be highly magnetostrictive and magnetically blocked at room temperature despite their nanometer-size. We describe here the use of the polyol process to synthesize cobalt ferrite (Co Fe O) nanoparticles with controlled size and composition and the study of the relationship between size and composition and the magnetic behavior. We used an improved synthesis of magnetostrictive Co Fe O NPs based on the forced hydrolysis of metallic salts in a polyol solvent, varying the fraction . Stoichiometric NPs ( = 1) are expected to be highly magnetostrictive while the sub-stoichiometric NPs (particularly for ≈ 0.7) are expected to be less magnetostrictive but to present a higher magnetocrystalline anisotropy constant, as previously observed in bulk cobalt ferrites. To control the size of the NPs, in order to overcome the superparamagnetic limit, as well as their chemical composition, in order to get the desired magnetomechanic properties, we carried out the reactions for two nominal precursor contents ( = 1 and 0.67), using two different solvents, i.e., triethylene glycol (TriEG) and tetraethylene glycol (TetEG), and three different durations of refluxing (3, 6 and 15 h). The structure, microstructure and composition of the resulting NPs were then investigated by using X-ray diffraction (XRD), transmission electron microscopy (TEM) and X-ray fluorescence spectroscopy (XRF), respectively. The magnetic properties were also evaluated using standard magnetometry. To measure the magnetostrictive response of the particles, the particles were sintered to dense pellets on which strain gauges were bonded, measuring the size variation radially, as a function of a dc magnetic field. We found two samples, the first one being stoichiometric and magnetostrictive, and the second one being sub-stoichiometric and presenting a higher magnetization, that are appropriate to be used as ferromagnetic building blocks in nanostructured magnetoelectric materials, particularly materials based on polymers. We show that the polyol solvent and the reaction time are two key parameters to control the size and the magnetic properties of the resulting nanoparticles. We believe that these results provide relevant insights to the design of efficient magnetic and magnetostrictive nanoparticles that can be further functionalized by coupling agents, to be contacted with piezoelectric polymers.
在由两种组分构成的外禀磁电材料中,直接磁电耦合源于外部磁场作用下磁致伸缩组分发生形状变化,从而在界面处产生机械应变传递。在此,两种组分之间界面的尺寸起着关键作用。因此,开发具有大表面积与体积比的纳米材料有助于满足这一要求。然而,磁性纳米颗粒(NPs)尽管尺寸为纳米级,但在室温下必须具有高磁致伸缩性且磁矩被冻结。我们在此描述了利用多元醇法合成尺寸和组成可控的钴铁氧体(CoFeO)纳米颗粒,并研究尺寸、组成与磁行为之间的关系。我们基于金属盐在多元醇溶剂中的强制水解,改进了磁致伸缩CoFeO NPs的合成方法,改变了摩尔分数。化学计量比的NPs(= 1)预计具有高磁致伸缩性,而非化学计量比的NPs(特别是≈ 0.7时)预计磁致伸缩性较低,但具有更高的磁晶各向异性常数,这与之前在块状钴铁氧体中观察到的情况一致。为了控制NPs的尺寸以克服超顺磁极限,以及控制其化学成分以获得所需的磁机械性能,我们针对两种标称前驱体含量(= 1和0.67),使用两种不同的溶剂,即三甘醇(TriEG)和四甘醇(TetEG),并进行三种不同时长(3、6和15小时)的回流反应。然后分别通过X射线衍射(XRD)、透射电子显微镜(TEM)和X射线荧光光谱(XRF)研究所得NPs的结构、微观结构和组成。还使用标准磁强计评估了磁性能。为了测量颗粒的磁致伸缩响应,将颗粒烧结成致密小球,并在上面粘贴应变片,测量其径向尺寸随直流磁场的变化。我们发现了两个样品,第一个是化学计量比且具有磁致伸缩性的,第二个是非化学计量比且具有较高磁化强度的,它们适合用作纳米结构磁电材料中的铁磁构建块,特别是基于聚合物的材料。我们表明多元醇溶剂和反应时间是控制所得纳米颗粒尺寸和磁性能的两个关键参数。我们相信这些结果为设计高效的磁性和磁致伸缩纳米颗粒提供了相关见解,这些纳米颗粒可通过偶联剂进一步功能化,以便与压电聚合物接触。