材料科学
六方晶系
铁氧体(磁铁)
微观结构
铁磁共振
尖晶石
磁畴
磁各向异性
磁导率
各向异性
损耗系数
核磁共振
介电损耗
电介质
单一领域
相对渗透率
共振(粒子物理)
光电子学
磁共振成像
平面的
热液循环
频域
复合材料
磁化
磁场
作者
Donglin He,Liang‐Rui Tan,Guo-Wu Wang,Longhui Xiong,Qinglin Li,Tao Wang
出处
期刊:Rare Metals
[Springer Science+Business Media]
日期:2025-10-13
卷期号:44 (12): 10632-10645
被引量:2
标识
DOI:10.1007/s12598-025-03613-3
摘要
Abstract The demands of ferrites with high permeability and low‐loss properties are significantly increased within the sub‐6 GHz band. However, traditional spinel and planar hexagonal ferrites, constrained by Snoek’s limit, struggle to meet the requirement of high operating frequency. This study introduces a novel approach by preparing textured CoRu‐substituted BaM hexaferrite incorporating Bi 2 O 3 additives, using high aspect‐ratio goethite precursors. Compared to ferrite synthesized through the conventional solid‐state reaction method, the optimized ferrite demonstrates remarkable improvements in maximum operating frequency (from 0.82 to 7.5 GHz) and performance factor PF (increasing from 23.7 to 98.2 GHz), while maintaining a low magnetic loss (~ 0.10). Magnetic spectrum analysis indicates that the goethite‐derived textured microstructure effectively increases the natural resonance frequency by enhancing the uniaxial magnetic anisotropy, facilitating the achievement of high operating frequency. Differential phase contrast (DPC) results show that adding Bi 2 O 3 broadens the magnetic domain and shifts the domain wall resonance peak to a lower frequency, distinguishing it from the natural resonance peak. Furthermore, compared with the pure dielectric material, the antenna designed using this ferrite exhibits a 17% reduction in size. This study presents a strategy for fabricating textured CoRu‐substituted BaM hexaferrites without the necessity for an external magnetic field and elucidating the regulation mechanism of microstructure on high‐frequency magnetic properties, and offering a novel magneto‐dielectric material that enhances uniaxial magnetic anisotropy while modifying the magnetic domain structure for the sub‐6 GHz band.
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