{"title":"硬/软交换耦合双层中界面原子相互扩散对成核场和能积的影响:一维微磁方法","authors":"P.Y. Wang , J. Wang , G.P. Zhao , Q. Zhao","doi":"10.1016/j.physb.2025.417565","DOIUrl":null,"url":null,"abstract":"<div><div>A one-dimensional (1D) analytical model is extended to study the magnetic properties of hard/soft exchange-coupled bilayers with the interface layer, focusing on SmCo/Fe and Nd<sub>2</sub>Fe<sub>14</sub>B/Fe systems. The results show that increasing the interface layer thickness <em>t</em><sup><em>i</em></sup> enhances the nucleation field <em>H</em><sub><em>N</em></sub><em>,</em> thereby increasing the maximum energy product (<em>BH</em>)<sub>max</sub>, while simultaneously reducing the pinning field <em>H</em><sub><em>P</em></sub>. For parallel SmCo(20 nm)/Fe(10 nm) bilayers, magnetic property changes with increasing <em>t</em><sup><em>i</em></sup> predicted by the 1D model align well with experiments at higher annealing temperatures. Complementary three-dimensional (3D) micromagnetic simulations confirm that <em>H</em><sub><em>N</em></sub> increases with <em>t</em><sup><em>i</em></sup> over a wide range of interface exchange energy constants, which shows in excellent agreement with the 1D calculated results over the investigated <em>t</em><sup><em>i</em></sup> range. Meanwhile, <em>H</em><sub><em>N</em></sub> also increases with the interface exchange coupling coefficient for each specific <em>t</em><sup><em>i</em></sup>. These findings indicate that appropriate interface atomic interdiffusion enhances the exchange coupling effect between the hard and soft phases and improves magnetic performance. The 1D model also identifies optimal interface layer thicknesses for maximizing (<em>BH</em>)<sub>max</sub> in both systems. Additionally, demagnetization curves of perpendicular Nd<sub>2</sub>Fe<sub>14</sub>B/Fe bilayers from the 1D model match 3D simulation results, verifying the model's accuracy. <strong>Importantly</strong>, the 1D model developed in this work is also applicable to hard/soft exchange-coupled trilayers with varying thicknesses and magnetic parameters in each layer. In contrast to our previous design, where atoms were assumed to diffuse from the hard phase into the soft phase, resulting in the interface layer being located on the soft phase side, this study considers mutual diffusion between the two phases, with the interface layer symmetrically distributed between them.</div></div>","PeriodicalId":20116,"journal":{"name":"Physica B-condensed Matter","volume":"715 ","pages":"Article 417565"},"PeriodicalIF":2.8000,"publicationDate":"2025-07-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The effect of the interface atomic interdiffusion on the nucleation field and energy product in hard/soft exchange-coupled bilayers: A one-dimensional micromagnetic approach\",\"authors\":\"P.Y. Wang , J. Wang , G.P. Zhao , Q. Zhao\",\"doi\":\"10.1016/j.physb.2025.417565\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>A one-dimensional (1D) analytical model is extended to study the magnetic properties of hard/soft exchange-coupled bilayers with the interface layer, focusing on SmCo/Fe and Nd<sub>2</sub>Fe<sub>14</sub>B/Fe systems. The results show that increasing the interface layer thickness <em>t</em><sup><em>i</em></sup> enhances the nucleation field <em>H</em><sub><em>N</em></sub><em>,</em> thereby increasing the maximum energy product (<em>BH</em>)<sub>max</sub>, while simultaneously reducing the pinning field <em>H</em><sub><em>P</em></sub>. For parallel SmCo(20 nm)/Fe(10 nm) bilayers, magnetic property changes with increasing <em>t</em><sup><em>i</em></sup> predicted by the 1D model align well with experiments at higher annealing temperatures. Complementary three-dimensional (3D) micromagnetic simulations confirm that <em>H</em><sub><em>N</em></sub> increases with <em>t</em><sup><em>i</em></sup> over a wide range of interface exchange energy constants, which shows in excellent agreement with the 1D calculated results over the investigated <em>t</em><sup><em>i</em></sup> range. Meanwhile, <em>H</em><sub><em>N</em></sub> also increases with the interface exchange coupling coefficient for each specific <em>t</em><sup><em>i</em></sup>. These findings indicate that appropriate interface atomic interdiffusion enhances the exchange coupling effect between the hard and soft phases and improves magnetic performance. The 1D model also identifies optimal interface layer thicknesses for maximizing (<em>BH</em>)<sub>max</sub> in both systems. Additionally, demagnetization curves of perpendicular Nd<sub>2</sub>Fe<sub>14</sub>B/Fe bilayers from the 1D model match 3D simulation results, verifying the model's accuracy. <strong>Importantly</strong>, the 1D model developed in this work is also applicable to hard/soft exchange-coupled trilayers with varying thicknesses and magnetic parameters in each layer. In contrast to our previous design, where atoms were assumed to diffuse from the hard phase into the soft phase, resulting in the interface layer being located on the soft phase side, this study considers mutual diffusion between the two phases, with the interface layer symmetrically distributed between them.</div></div>\",\"PeriodicalId\":20116,\"journal\":{\"name\":\"Physica B-condensed Matter\",\"volume\":\"715 \",\"pages\":\"Article 417565\"},\"PeriodicalIF\":2.8000,\"publicationDate\":\"2025-07-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physica B-condensed Matter\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0921452625006829\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, CONDENSED MATTER\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physica B-condensed Matter","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0921452625006829","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
The effect of the interface atomic interdiffusion on the nucleation field and energy product in hard/soft exchange-coupled bilayers: A one-dimensional micromagnetic approach
A one-dimensional (1D) analytical model is extended to study the magnetic properties of hard/soft exchange-coupled bilayers with the interface layer, focusing on SmCo/Fe and Nd2Fe14B/Fe systems. The results show that increasing the interface layer thickness ti enhances the nucleation field HN, thereby increasing the maximum energy product (BH)max, while simultaneously reducing the pinning field HP. For parallel SmCo(20 nm)/Fe(10 nm) bilayers, magnetic property changes with increasing ti predicted by the 1D model align well with experiments at higher annealing temperatures. Complementary three-dimensional (3D) micromagnetic simulations confirm that HN increases with ti over a wide range of interface exchange energy constants, which shows in excellent agreement with the 1D calculated results over the investigated ti range. Meanwhile, HN also increases with the interface exchange coupling coefficient for each specific ti. These findings indicate that appropriate interface atomic interdiffusion enhances the exchange coupling effect between the hard and soft phases and improves magnetic performance. The 1D model also identifies optimal interface layer thicknesses for maximizing (BH)max in both systems. Additionally, demagnetization curves of perpendicular Nd2Fe14B/Fe bilayers from the 1D model match 3D simulation results, verifying the model's accuracy. Importantly, the 1D model developed in this work is also applicable to hard/soft exchange-coupled trilayers with varying thicknesses and magnetic parameters in each layer. In contrast to our previous design, where atoms were assumed to diffuse from the hard phase into the soft phase, resulting in the interface layer being located on the soft phase side, this study considers mutual diffusion between the two phases, with the interface layer symmetrically distributed between them.
期刊介绍:
Physica B: Condensed Matter comprises all condensed matter and material physics that involve theoretical, computational and experimental work.
Papers should contain further developments and a proper discussion on the physics of experimental or theoretical results in one of the following areas:
-Magnetism
-Materials physics
-Nanostructures and nanomaterials
-Optics and optical materials
-Quantum materials
-Semiconductors
-Strongly correlated systems
-Superconductivity
-Surfaces and interfaces