在铁磁性8-Pmmn基结中进行电子传输和旋谷偏振
Yemby Yajaida Huamani-Tapia1, Isaac Rodríguez-Vargas2, José Guadalupe Rojas-Briseño3
1Unidad Académica de Ciencia y Tecnología de la Luz y la Materia, Universidad Autonoma de Zacatecas, Circuito Marie Curie S/N, Parque de Ciencia y Tecnología QUANTUM Ciudad del Conocimiento, Zacatecas, Zacatecas, 98160, MEXICO.
Journal of physics. Condensed matter : an Institute of Physics journal
|September 2, 2025
概括
铁磁 8-Pmmn 基结可以控制旋转和谷极化. 同时应用磁场和磁化可以实现完美的旋转和谷极化,为旋转和谷极化设备铺平了道路.
科学领域:
- 凝聚物质物理学
- 材料科学
- 纳米技术
背景情况:
- 8-Pmmn是一种具有独特电子特性的二维材料.
- 它的倾斜带结构支持像斜克莱恩道这样的现象.
- 门接口可以控制旋转谷的电子传输.
研究的目的:
- 在铁磁 8-Pmmn 基结中研究旋转和谷极化.
- 探索磁化和外部磁场的影响.
- 确定旋转和山谷应用的潜力.
主要方法:
- 在8-Pmmn基结中旋转和谷运输的理论分析.
- 考虑横向波向量,静电门和磁门.
- 同时分析磁化和外部磁场.
主要成果:
- 磁化本身就产生了自旋两极化,而不是谷两极化.
- 外部磁场会增加山谷的退化,从而使山谷两极化.
- 同时的磁场和磁化破坏了旋转谷的退化,
- 斜门的位置增强了旋转极化区域.
结论:
- 铁磁 8-Pmmn 基结提供可调节的旋转和谷极化.
- 精确控制磁场和电场是关键.
- 这些连接对未来的自旋电子和谷电子设备来说是有前途的.
相关概念视频
P-N junction
673
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
673
Biasing of Metal-Semiconductor Junctions
331
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
331
Metal-Semiconductor Junctions
505
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
505
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
Biasing of P-N Junction
839
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
839
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


