从合成 SrRuO3晶体中异常霍尔效应的磁性异构的维度工程3
Seung Gyo Jeong1, Seong Won Cho2, Sehwan Song3
1Department of Physics, Sungkyunkwan University, Suwon 16419, Korea.
Nano letters
|June 3, 2024
概括
原子薄的氧化物异构结构具有可调节的磁性. 工程 SrRuO3/SrTiO3 超级网格显著增强了磁性异构性和强制场,用于先进的自旋电子学.
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
- 这就是Spintronics.
背景情况:
- 原子薄的相关异构结构对于量子磁相和下一代自旋电子技术至关重要.
- 之前的研究主要集中在范德瓦尔斯系统的磁性异性学研究.
研究的目的:
- 探究在长长的相关氧化物中维度的影响,直至单层极限.
- 在氧化物超级晶格中探索结构性,磁性和轨道异质.
- 了解在缩小尺寸中增强磁性异构性背后的机制.
主要方法:
- 使用SrRuO3 (相关铁磁) 和SrTiO3 (非磁) 层制造氧化物超级网格.
- 在SrRuO3层厚度的系统变化下降到单层极限.
- 结构性质,磁性质和异常霍尔效应的表征.
主要成果:
- 观察到调制的铁磁行为与SrRuO3厚度的变化.
- 对于三单元细胞厚的SrRuO3层,强迫场的显著1500%的改善,由异常的霍尔效应证明.
- 系统调节格子结构和轨道杂交,与增强的磁性异质相对应.
结论:
- 经轴氧化物异构结构提供了一个可调的平台,用于设计磁性异构.
- 维度在调节磁性和轨道性质方面发挥着至关重要的作用.
- 结果为设计合成磁性晶体提供了洞察力,为旋转应用提供了定制的旋转顺序.
更多相关视频
06:49Radio Frequency Magnetron Sputtering of GdBa2Cu3O7âˆ'ÃŽ ´/ La0.67Sr0.33MnO3 Quasi-bilayer Films on SrTiO3 STO Single-crystal Substrates
Published on: April 12, 2019
7.6K
11:54Growth and Electrostatic/chemical Properties of Metal/LaAlO3/SrTiO3 Heterostructures
Published on: February 8, 2018
10.3K
相关概念视频
The Hall Effect
2.3K
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
2.3K
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
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
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
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
Diamagnetism
2.4K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.4K
