Insights into the structural and microscopic origin of magnetic and optical properties of monodispersed γ-Fe2O3, ZnO, γ-Fe2−2xZn2xO3 and γ-Fe2O3@ZnO nanostructures†

IF 2.6 3区 化学 Q2 CHEMISTRY, MULTIDISCIPLINARY
CrystEngComm Pub Date : 2025-05-21 DOI:10.1039/D5CE00317B
Ruchi Agrawal, Manas Srivastava, Debashish Sarkar and Raghumani Singh Ningthoujam
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引用次数: 0

Abstract

Monodispersed γ-Fe2O3, ZnO, γ-Fe2−2xZn2xO3 (substitution, SUB) and γ-Fe2O3@ZnO (core@shell, CS) nanoparticles were synthesized via a thermolysis method, and their changes in optical and magnetic behaviour were investigated. γ-Fe2O3, γ-Fe2−2xZn2xO3 and γ-Fe2O3@ZnO nanoparticles were crystallized in cubic structure, whereas ZnO was found to be amorphous. γ-Fe2O3 nanoparticles were spherical, whereas SUB and CS nanoparticles were nanorods. In the magnetization versus applied magnetic field (MH curve) study, γ-Fe2O3 nanoparticles were superparamagnetic at room temperature and ferromagnetic at 5 K. At room temperature, SUB nanoparticles showed paramagnetic behaviour at an applied magnetic field below 2500 Oe, and above 2500 Oe, these nanoparticles exhibited diamagnetic behaviour, which can be attributed to the contribution of ZnFe2O4 and ZnO. At 5 K, SUB nanoparticles exhibited paramagnetic behaviour. CS nanoparticles showed paramagnetic/diamagnetic behaviour at room temperature but showed weak ferromagnetic behaviour at 5 K. This can be represented as small size core γ-Fe2O3@interface ZnFe2O4@shell ZnO. ZnO nanoparticles were diamagnetic at room temperature, but it became paramagnetic at 5 K. At zero-field cooled and field-cooled curves, γ-Fe2O3 nanoparticles showed a blocking temperature (TB) at 210 K. ZnO, SUB and CS nanoparticles showed a peak at 50–60 K in the zero-field cooled curve, which suggested the presence of antiferromagnetic interactions in these materials. In the photoluminescence study, luminescence intensity was highest in ZnO, followed by CS, SUB and γ-Fe2O3. In terms of the proximity effect, SUB could be considered as ZnFe2O4/ZnO/FeO (mixture), whereas CS could be considered as γ-Fe2O3@ZnFe2O4@ZnO (core@interface@shell). The decrease in photoluminescence intensity was owing to the presence of magnetic impurities, which was supported by the decay lifetime study. The relations between crystal structure, microstructures, magnetic and optical properties are studied in this work.

Abstract Image

单分散γ- fe2o3、ZnO、γ- fe2−2xZn2xO3和γ-Fe2O3@ZnO纳米结构†磁性和光学性质的结构和微观起源
采用热裂解法制备了单分散的γ- fe2o3、ZnO、γ- fe2−2xZn2xO3(取代,SUB)和γ-Fe2O3@ZnO (core@shell, CS)纳米粒子,研究了它们的光学和磁性行为变化。γ- fe2o3、γ- fe2−2xZn2xO3和γ-Fe2O3@ZnO纳米颗粒呈立方结构结晶,而ZnO则呈非晶态。γ-Fe2O3纳米颗粒呈球形,而SUB和CS纳米颗粒呈纳米棒状。在磁化强度与外加磁场的关系(M-H曲线)研究中,γ-Fe2O3纳米颗粒在室温下具有超顺磁性,在5k时具有铁磁性。在室温下,SUB纳米粒子在外加磁场低于2500 Oe时表现出顺磁性,而在外加磁场高于2500 Oe时表现出反磁性,这主要归因于ZnFe2O4和ZnO的贡献。在5 K时,SUB纳米颗粒表现出顺磁性。CS纳米颗粒在室温下表现为顺磁性/抗磁性,在5k时表现为弱铁磁性。这可以表示为小尺寸的核心γ-Fe2O3@interface ZnFe2O4@shell ZnO。ZnO纳米粒子在室温下具有抗磁性,但在5k时变为顺磁性。在零场冷却和场冷却曲线上,γ-Fe2O3纳米颗粒在210 K时表现出阻滞温度(TB)。ZnO、SUB和CS纳米粒子的零场冷却曲线在50 ~ 60 K处出现峰值,表明这些材料中存在反铁磁相互作用。在光致发光研究中,ZnO的发光强度最高,其次是CS、SUB和γ-Fe2O3。在接近效应方面,SUB可以考虑为ZnFe2O4/ZnO/FeO(混合物),而CS可以考虑为γ-Fe2O3@ZnFe2O4@ZnO (core@interface@壳)。光致发光强度的降低是由于磁性杂质的存在,这一点得到了衰变寿命研究的支持。研究了晶体结构、显微结构、磁性和光学性能之间的关系。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CrystEngComm
CrystEngComm 化学-化学综合
CiteScore
5.50
自引率
9.70%
发文量
747
审稿时长
1.7 months
期刊介绍: Design and understanding of solid-state and crystalline materials
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