Jessica MacDougall, Asuka Namai, Onno Strolka and Shin-ichi Ohkoshi
{"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":5.2000,"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}
引用次数: 0
Abstract
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.