• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

连续梯度铁磁体中纳米尺度磁性能的调制。

Modulation of Magnetic Properties at the Nanometer Scale in Continuously Graded Ferromagnets.

作者信息

Fallarino Lorenzo, Riego Patricia, Kirby Brian J, Miller Casey W, Berger Andreas

机构信息

CIC nanoGUNE, Tolosa Hiribidea 76, E-20018 Donostia-San Sebastian, Spain.

Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, Bautzner Landstrasse 400, 01328 Dresden, Germany.

出版信息

Materials (Basel). 2018 Feb 6;11(2):251. doi: 10.3390/ma11020251.

DOI:10.3390/ma11020251
PMID:29415524
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5848948/
Abstract

: Ferromagnetic alloy materials with designed composition depth profiles provide an efficient route for the control of magnetism at the nanometer length scale. In this regard, cobalt-chromium and cobalt-ruthenium alloys constitute powerful model systems. They exhibit easy-to-tune magnetic properties such as saturation magnetization and Curie temperature while preserving their crystalline structure over a wide composition range. In order to demonstrate this materials design potential, we have grown a series of graded Co₁Cr and Co₁Ru (1010) epitaxial thin films, with and following predefined concentration profiles. Structural analysis measurements verify the epitaxial nature and crystallographic quality of our entire sample sets, which were designed to exhibit in-plane -axis orientation and thus a magnetic in-plane easy axis to achieve suppression of magnetostatic domain generation. Temperature and field-dependent magnetic depth profiles have been measured by means of polarized neutron reflectometry. In both investigated structures, and are found to vary as a function of depth in accordance with the predefined compositional depth profiles. Our Co₁Ru sample structures, which exhibit very steep material gradients, allow us to determine the localization limit for compositionally graded materials, which we find to be of the order of 1 nm. The Co₁Cr systems show the expected U-shaped and depth profiles, for which these specific samples were designed. The corresponding temperature dependent magnetization profile is then utilized to control the coupling along the film depth, which even allows for a sharp onset of decoupling of top and bottom sample parts at elevated temperatures.

摘要

具有设计成分深度分布的铁磁合金材料为在纳米长度尺度上控制磁性提供了一条有效途径。在这方面,钴铬合金和钴钌合金构成了强大的模型体系。它们展现出易于调节的磁性,如饱和磁化强度和居里温度,同时在很宽的成分范围内保持其晶体结构。为了证明这种材料设计潜力,我们生长了一系列具有预定义浓度分布的梯度Co₁Cr和Co₁Ru(1010)外延薄膜。结构分析测量验证了我们整个样品集的外延性质和晶体质量,这些样品集被设计为具有面内 - 轴取向,从而具有面内易磁化轴以抑制静磁畴的产生。通过极化中子反射测量法测量了温度和磁场依赖的磁性深度分布。在这两种研究结构中,发现 和 随深度变化,符合预定义的成分深度分布。我们的Co₁Ru样品结构具有非常陡峭的材料梯度,这使我们能够确定成分渐变材料的局域化极限,我们发现其约为1纳米。Co₁Cr体系呈现出预期的U形 和 深度分布,这些特定样品就是为此设计的。然后利用相应的温度依赖磁化分布来控制沿薄膜深度的耦合,这甚至允许在高温下顶部和底部样品部分的解耦急剧开始。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/10a26fd290d5/materials-11-00251-g016.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/cdf90e207538/materials-11-00251-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/66dcda17d85e/materials-11-00251-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/41cbfa826aa6/materials-11-00251-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/c1615d1b15aa/materials-11-00251-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/059a63d53e68/materials-11-00251-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/2685bf5a64cc/materials-11-00251-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/c1823601bfbe/materials-11-00251-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/69356280640d/materials-11-00251-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/3c1414bef263/materials-11-00251-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/aada19bb723b/materials-11-00251-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/6c0600773887/materials-11-00251-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/e00ac284c66f/materials-11-00251-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/848e529a8a03/materials-11-00251-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/af937c30fb3e/materials-11-00251-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/ae8362687f1f/materials-11-00251-g015.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/10a26fd290d5/materials-11-00251-g016.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/cdf90e207538/materials-11-00251-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/66dcda17d85e/materials-11-00251-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/41cbfa826aa6/materials-11-00251-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/c1615d1b15aa/materials-11-00251-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/059a63d53e68/materials-11-00251-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/2685bf5a64cc/materials-11-00251-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/c1823601bfbe/materials-11-00251-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/69356280640d/materials-11-00251-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/3c1414bef263/materials-11-00251-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/aada19bb723b/materials-11-00251-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/6c0600773887/materials-11-00251-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/e00ac284c66f/materials-11-00251-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/848e529a8a03/materials-11-00251-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/af937c30fb3e/materials-11-00251-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/ae8362687f1f/materials-11-00251-g015.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3f45/5848948/10a26fd290d5/materials-11-00251-g016.jpg

相似文献

1
Modulation of Magnetic Properties at the Nanometer Scale in Continuously Graded Ferromagnets.连续梯度铁磁体中纳米尺度磁性能的调制。
Materials (Basel). 2018 Feb 6;11(2):251. doi: 10.3390/ma11020251.
2
Graded magnetic materials.梯度磁性材料。
J Phys D Appl Phys. 2021;54(30). doi: 10.1088/1361-6463/abfad3.
3
Structural, magnetic and magnetocaloric effects in epitaxial LaBaTiMnO ferromagnetic thin films grown on 001-oriented SrTiO substrates.在001取向的SrTiO衬底上生长的外延LaBaTiMnO铁磁薄膜中的结构、磁性和磁热效应。
Dalton Trans. 2016 Sep 27;45(38):15034-15040. doi: 10.1039/c6dt01914e.
4
Interface biquadratic coupling and magnon scattering in exchange-biased ferromagnetic thin films grown on epitaxial FeF2.外延生长在 FeF2 上的交换偏置铁磁薄膜中的界面二次型耦合和磁子散射
J Phys Condens Matter. 2012 May 9;24(18):186001. doi: 10.1088/0953-8984/24/18/186001. Epub 2012 Apr 5.
5
Magnetic and structural depth profiles of Heusler alloy CoFeAlSi epitaxial films on Si(1 1 1).硅(111)衬底上赫斯勒合金CoFeAlSi外延膜的磁性和结构深度分布
J Phys Condens Matter. 2018 Feb 14;30(6):065801. doi: 10.1088/1361-648X/aaa4c8.
6
Modifying Critical Exponents of Magnetic Phase Transitions via Nanoscale Materials Design.通过纳米级材料设计改变磁相变的临界指数
Phys Rev Lett. 2021 Oct 1;127(14):147201. doi: 10.1103/PhysRevLett.127.147201.
7
Magnetic nonuniformity and thermal hysteresis of magnetism in a manganite thin film.锰氧化物薄膜中磁性的磁各向异性和热滞现象。
Phys Rev Lett. 2012 Feb 17;108(7):077207. doi: 10.1103/PhysRevLett.108.077207.
8
Magnetic properties of epitaxial Heusler alloy (Co(2/3)Fe(1/3))(3+x)Si(1-x)/GaAs(001) hybrid structures.外延赫斯勒合金(Co(2/3)Fe(1/3))(3+x)Si(1-x)/GaAs(001)混合结构的磁性
J Phys Condens Matter. 2006 Jul 5;18(26):6101-8. doi: 10.1088/0953-8984/18/26/028. Epub 2006 Jun 19.
9
Structural and Magnetic Properties of LaCoO3/SrTiO3 Multilayers.LaCoO3/SrTiO3 多层结构的结构和磁性。
ACS Appl Mater Interfaces. 2016 Jul 20;8(28):18328-33. doi: 10.1021/acsami.6b03756. Epub 2016 Jul 11.
10
Complex Evolution of Built-in Potential in Compositionally-Graded PbZr(1-x)Ti(x)O3 Thin Films.组分梯度 PbZr(1-x)Ti(x)O3 薄膜中内置电势的复杂演变。
ACS Nano. 2015 Jul 28;9(7):7332-42. doi: 10.1021/acsnano.5b02289. Epub 2015 Jul 10.

引用本文的文献

1
Graded magnetic materials.梯度磁性材料。
J Phys D Appl Phys. 2021;54(30). doi: 10.1088/1361-6463/abfad3.
2
Spin-Wave Channeling in Magnetization-Graded Nanostrips.磁化梯度纳米条带中的自旋波通道效应
Nanomaterials (Basel). 2022 Aug 14;12(16):2785. doi: 10.3390/nano12162785.

本文引用的文献

1
Spatial Evolution of the Ferromagnetic Phase Transition in an Exchange Graded Film.交换梯度薄膜中铁磁相变的空间演化
Phys Rev Lett. 2016 Jan 29;116(4):047203. doi: 10.1103/PhysRevLett.116.047203.
2
Origin, development, and future of spintronics (Nobel Lecture).自旋电子学的起源、发展及未来(诺贝尔演讲)
Angew Chem Int Ed Engl. 2008;47(32):5956-67. doi: 10.1002/anie.200801093.
3
Giant room-temperature magnetoresistance in single-crystal Fe/MgO/Fe magnetic tunnel junctions.单晶Fe/MgO/Fe磁性隧道结中的巨室温磁电阻
Nat Mater. 2004 Dec;3(12):868-71. doi: 10.1038/nmat1257. Epub 2004 Oct 31.
4
Giant energy product in nanostructured two-phase magnets.纳米结构两相磁体中的巨型能量积
Phys Rev B Condens Matter. 1993 Dec 1;48(21):15812-15816. doi: 10.1103/physrevb.48.15812.