在四角形Mn-Rh-Ir-Sn反向的海斯勒化合物中磁性调性
1Department of Metallurgical and Materials Engineering, Colorado School of Mines, Golden, CO 80401, United States of America.
概括
控制材料中复杂的磁性结构是一项挑战. 这项研究探讨了Mn-Rh-Sn与Ir的替代,发现它调整磁相,但由于狭窄的组成窗口,没有预测的复杂非对线状态.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 磁力学 磁力学 是一种
背景情况:
- 控制复杂的磁性结构 (非对线性,纳米级) 仍然是一个重大挑战.
- 调整Dzyaloshinskii-Moriya相互作用到四边形反向的单轴磁性异性变性比,HEUSLERS可以访问各种磁性状态 (铁磁,螺旋,反螺旋相).
研究的目的:
- 在Mn-Rh-Sn系统中研究磁相行为的可调性.
- 探索 (Ir) 替代对Rh基结构的影响.
- 确定复杂的非对线磁相是否可以通过组合调来访问.
主要方法:
- 在Mn-Rh-Sn的Rh基结构中系统地替代 (Ir).
- 对磁相转换和磁交换合的分析.
- 磁性结构的特征 敏感度对静脉测量.
主要成果:
- 替代成功调整了Mn-Rh-Sn系统的磁相行为.
- 替代导致铁磁交换合的增加,以牺牲反铁磁合为代价.
- 预测的复杂的非线性磁相 (螺旋,反螺旋) 并没有被观察到.
结论:
- Mn-Rh-Sn的磁相行为可以通过替代进行调整.
- 观察预测的复杂磁相的困难归因于它们在批量样本中形成的极其狭窄的组成窗口.
- 复杂的磁性结构对材料固态度非常敏感,使实证发现复杂化.
相关概念视频
Colors and Magnetism
11.7K
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
11.7K
Ferromagnetism
2.4K
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...
2.4K
Valence Bond Theory
8.6K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
8.6K
Paramagnetism
2.5K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
2.5K
Atomic Nuclei: Magnetic Resonance
658
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
658
Magnetic Susceptibility and Permeability
1.1K
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...
1.1K


