Jessica MacDougall, Asuka Namai, Onno Strolka and Shin-ichi Ohkoshi
{"title":"mn取代效应对ε-Fe2O3纳米粒子磁性和零场铁磁共振特性的影响","authors":"Jessica MacDougall, Asuka Namai, Onno Strolka and Shin-ichi Ohkoshi","doi":"10.1039/D4MA00927D","DOIUrl":null,"url":null,"abstract":"<p >Metal substitution is an important way to tune the magnetic properties of ferrites. In the present study, to investigate the effects of Mn substitution on the magnetic properties and millimeter wave absorption properties on ε-Fe<small><sub>2</sub></small>O<small><sub>3</sub></small> for the first time, Mn-substituted epsilon iron oxides, ε-Mn<small><sub><em>x</em></sub></small>Fe<small><sub>2−<em>x</em></sub></small>O<small><sub>3−<em>x</em>/2</sub></small> (<em>x</em> = 0 (<strong>Mn0</strong>), 0.10 (<strong>Mn1</strong>), and 0.20 (<strong>Mn2</strong>)) were synthesized by sintering iron oxide hydroxide with manganese hydroxide in a silica matrix. Transmission electron microscopy shows particle sizes of 18.7 ± 5.8 nm (<strong>Mn0</strong>), 19.0 ± 6.2 nm (<strong>Mn1</strong>), and 19.8 ± 6.7 nm (<strong>Mn2</strong>). Energy dispersive X-ray spectroscopy confirms a uniform manganese distribution across all particles, while the powder X-ray diffraction patterns demonstrate that ε-Mn<small><sub><em>x</em></sub></small>Fe<small><sub>2−<em>x</em></sub></small>O<small><sub>3−<em>x</em>/2</sub></small> has an orthorhombic crystal structure with a space group of <em>Pna</em>2<small><sub>1</sub></small> (<em>e.g.</em>, the lattice constants in <strong>Mn2</strong> are <em>a</em> = 5.1031(4) Å, <em>b</em> = 8.7759(8) Å, and <em>c</em> = 9.4661(7) Å). As the Mn substitution ratio increases, the Curie temperature decreases from 487 K (<strong>Mn0</strong>) to 469 K (<strong>Mn2</strong>). As for the magnetic properties at 300 K, the coercive field increases from 17.2 kOe (<strong>Mn0</strong>) to 18.2 kOe (<strong>Mn2</strong>), while the saturation magnetisation decreases from 17.1 emu g<small><sup>−1</sup></small> (<strong>Mn0</strong>) to 13.9 emu g<small><sup>−1</sup></small> (<strong>Mn2</strong>), with increasing substitution ratio. Terahertz time-domain spectroscopy demonstrates that the samples exhibit electromagnetic wave absorption in the millimetre-wave region, due to zero-field ferromagnetic resonance. As the Mn substitution ratio increases, the resonance frequency increases from 174 GHz (<strong>Mn0</strong>) to 182 GHz (<strong>Mn1</strong>) and 187 GHz (<strong>Mn2</strong>). Due to the substitution of Fe<small><sup>3+</sup></small> with Mn<small><sup>2+</sup></small>, the saturation magnetisation decreases and the coercive field and the resonance frequency increase.</p>","PeriodicalId":18242,"journal":{"name":"Materials Advances","volume":" 3","pages":" 969-976"},"PeriodicalIF":5.8000,"publicationDate":"2024-12-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2025/ma/d4ma00927d?page=search","citationCount":"0","resultStr":"{\"title\":\"Mn-substitution effects on the magnetic and zero-field ferromagnetic resonance properties of ε-Fe2O3 nanoparticles†\",\"authors\":\"Jessica MacDougall, Asuka Namai, Onno Strolka and Shin-ichi Ohkoshi\",\"doi\":\"10.1039/D4MA00927D\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Metal substitution is an important way to tune the magnetic properties of ferrites. In the present study, to investigate the effects of Mn substitution on the magnetic properties and millimeter wave absorption properties on ε-Fe<small><sub>2</sub></small>O<small><sub>3</sub></small> for the first time, Mn-substituted epsilon iron oxides, ε-Mn<small><sub><em>x</em></sub></small>Fe<small><sub>2−<em>x</em></sub></small>O<small><sub>3−<em>x</em>/2</sub></small> (<em>x</em> = 0 (<strong>Mn0</strong>), 0.10 (<strong>Mn1</strong>), and 0.20 (<strong>Mn2</strong>)) were synthesized by sintering iron oxide hydroxide with manganese hydroxide in a silica matrix. Transmission electron microscopy shows particle sizes of 18.7 ± 5.8 nm (<strong>Mn0</strong>), 19.0 ± 6.2 nm (<strong>Mn1</strong>), and 19.8 ± 6.7 nm (<strong>Mn2</strong>). Energy dispersive X-ray spectroscopy confirms a uniform manganese distribution across all particles, while the powder X-ray diffraction patterns demonstrate that ε-Mn<small><sub><em>x</em></sub></small>Fe<small><sub>2−<em>x</em></sub></small>O<small><sub>3−<em>x</em>/2</sub></small> has an orthorhombic crystal structure with a space group of <em>Pna</em>2<small><sub>1</sub></small> (<em>e.g.</em>, the lattice constants in <strong>Mn2</strong> are <em>a</em> = 5.1031(4) Å, <em>b</em> = 8.7759(8) Å, and <em>c</em> = 9.4661(7) Å). As the Mn substitution ratio increases, the Curie temperature decreases from 487 K (<strong>Mn0</strong>) to 469 K (<strong>Mn2</strong>). As for the magnetic properties at 300 K, the coercive field increases from 17.2 kOe (<strong>Mn0</strong>) to 18.2 kOe (<strong>Mn2</strong>), while the saturation magnetisation decreases from 17.1 emu g<small><sup>−1</sup></small> (<strong>Mn0</strong>) to 13.9 emu g<small><sup>−1</sup></small> (<strong>Mn2</strong>), with increasing substitution ratio. Terahertz time-domain spectroscopy demonstrates that the samples exhibit electromagnetic wave absorption in the millimetre-wave region, due to zero-field ferromagnetic resonance. As the Mn substitution ratio increases, the resonance frequency increases from 174 GHz (<strong>Mn0</strong>) to 182 GHz (<strong>Mn1</strong>) and 187 GHz (<strong>Mn2</strong>). Due to the substitution of Fe<small><sup>3+</sup></small> with Mn<small><sup>2+</sup></small>, the saturation magnetisation decreases and the coercive field and the resonance frequency increase.</p>\",\"PeriodicalId\":18242,\"journal\":{\"name\":\"Materials Advances\",\"volume\":\" 3\",\"pages\":\" 969-976\"},\"PeriodicalIF\":5.8000,\"publicationDate\":\"2024-12-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://pubs.rsc.org/en/content/articlepdf/2025/ma/d4ma00927d?page=search\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Materials Advances\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2025/ma/d4ma00927d\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Materials Advances","FirstCategoryId":"1085","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/ma/d4ma00927d","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
金属取代是调整铁氧体磁性能的重要手段。为了研究Mn取代对ε-Fe2O3磁性能和毫米波吸收性能的影响,本文首次在二氧化硅基体上用氢氧化铁和氢氧化锰烧结法制备了Mn取代ε-Fe2O3氧化铁ε-MnxFe2−xO3−x/2 (x = 0 (Mn0), 0.10 (Mn1)和0.20 (Mn2))。透射电镜显示,Mn0、mnn1和Mn2的粒径分别为18.7±5.8 nm、19.0±6.2 nm和19.8±6.7 nm。能量色散x射线谱图证实了所有颗粒中锰的均匀分布,而粉末x射线衍射图表明ε-MnxFe2−xO3−x/2具有正交晶体结构,其空间群为Pna21(例如,Mn2的晶格常数为a = 5.1031(4) Å, b = 8.7759(8) Å, c = 9.4661(7) Å)。随着Mn取代率的增加,居里温度从487 K (Mn0)降低到469 K (Mn2)。在300 K时,随着取代比的增加,顽固性磁场从17.2 kOe (Mn0)增大到18.2 kOe (Mn2),饱和磁化强度从17.1 emu g−1 (Mn0)减小到13.9 emu g−1 (Mn2)。太赫兹时域光谱表明,由于零场铁磁共振,样品在毫米波区域表现出电磁波吸收。随着Mn取代比的增加,谐振频率从174 GHz (Mn0)增加到182 GHz (Mn1)和187 GHz (Mn2)。由于Fe3+被Mn2+取代,饱和磁化强度降低,矫顽力场和共振频率增加。
Mn-substitution effects on the magnetic and zero-field ferromagnetic resonance properties of ε-Fe2O3 nanoparticles†
Metal substitution is an important way to tune the magnetic properties of ferrites. In the present study, to investigate the effects of Mn substitution on the magnetic properties and millimeter wave absorption properties on ε-Fe2O3 for the first time, Mn-substituted epsilon iron oxides, ε-MnxFe2−xO3−x/2 (x = 0 (Mn0), 0.10 (Mn1), and 0.20 (Mn2)) were synthesized by sintering iron oxide hydroxide with manganese hydroxide in a silica matrix. Transmission electron microscopy shows particle sizes of 18.7 ± 5.8 nm (Mn0), 19.0 ± 6.2 nm (Mn1), and 19.8 ± 6.7 nm (Mn2). Energy dispersive X-ray spectroscopy confirms a uniform manganese distribution across all particles, while the powder X-ray diffraction patterns demonstrate that ε-MnxFe2−xO3−x/2 has an orthorhombic crystal structure with a space group of Pna21 (e.g., the lattice constants in Mn2 are a = 5.1031(4) Å, b = 8.7759(8) Å, and c = 9.4661(7) Å). As the Mn substitution ratio increases, the Curie temperature decreases from 487 K (Mn0) to 469 K (Mn2). As for the magnetic properties at 300 K, the coercive field increases from 17.2 kOe (Mn0) to 18.2 kOe (Mn2), while the saturation magnetisation decreases from 17.1 emu g−1 (Mn0) to 13.9 emu g−1 (Mn2), with increasing substitution ratio. Terahertz time-domain spectroscopy demonstrates that the samples exhibit electromagnetic wave absorption in the millimetre-wave region, due to zero-field ferromagnetic resonance. As the Mn substitution ratio increases, the resonance frequency increases from 174 GHz (Mn0) to 182 GHz (Mn1) and 187 GHz (Mn2). Due to the substitution of Fe3+ with Mn2+, the saturation magnetisation decreases and the coercive field and the resonance frequency increase.