放射線条件下におけるbcc-Feの磁性アニソトロピーエネルギーの変化に関する第一原理の研究
Chunhui Li1, Wenjiang Qiang2, Bingxin Huang1
1University of Science and Technology Beijing, No. 76 Xueyuan South Road, Haidian Distr, Beijing, 100083, CHINA.
まとめ
セルフ・インタースティシャル・アトム (SIA) は,bcc-Feの磁性アニソトロピーエネルギー (MAE) を著しく高め,特にSIAがMnである場合. SIA近くの溶質原子分離はMAEを減少させ,磁気材料に対する放射線効果の洞察を提供します.
科学分野:
- 材料科学
- 凝縮物質物理学
- コンピュータ材料科学
背景:
- セルフ・インタースティシャル・アトム (SIA) は,結晶格子における点欠陥である.
- マグネティック・アニゾトロピー・エネルギー (MAE) は,磁気材料の応用において極めて重要です.
- 磁気特性に対する欠陥の影響を理解することは,材料の開発に不可欠です.
研究 の 目的:
- 身体中心の立方体鉄 (bcc-Fe) のMAEに対するSIAの影響を調査する.
- SIAによって引き起こされるMAEの根本的なメカニズムを解明する.
- 特定の溶質原子 (Mn) の役割とMAEに対する分離効果を探求する.
主な方法:
- 密度関数理論に基づく第一原理の計算
- 電子構造とスピン軌道結合 (SOC) の貢献の分析.
- MAEの起源を理解するために第二次乱射理論の適用.
主要な成果:
- SIAはbcc-FeのMAEを大幅に高めています.
- SIAとしてMnの存在は,より顕著なMAE強化につながります.
- SIAは局所的な原子構造と軌道交配を変化させ,SOCマトリックス要素に影響を与える.
- SIA欠陥の近くの溶液原子の分離はMAEを減らすことができます.
結論:
- SIA欠陥はbcc-FeにおけるMAEの重要な調節因子である.
- この研究は,SIAによるMAE変化のメカニズム的な理解を提供します.
- 発見は,放射性物質の磁気特性を予測し制御するための理論的基礎を提供します.
関連する概念動画
Ferromagnetism
2.5K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.5K
π Electron Effects on Chemical Shift: Overview
1.1K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.1K
Magnetic Susceptibility and Permeability
1.4K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.4K
Diamagnetic Shielding of Nuclei: Local Diamagnetic Current
958
An applied magnetic field causes the electrons present in the molecule to circulate, setting up a local diamagnetic current within the molecule. The local diamagnetic current arising from circulating sigma-bonding electrons induces a magnetic field, Blocal that opposes the applied magnetic field, B0. The effective magnetic field experienced by these nuclei is given by the difference between the applied and local magnetic fields in a phenomenon called local diamagnetic shielding. Essentially,...
958
Atomic Nuclei: Nuclear Relaxation Processes
718
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
718
Atomic Nuclei: Nuclear Magnetic Moment
1.4K
All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
1.4K


