在一个非弹道式旋转场效应晶体管中控制电注入旋转的控制旋转
Franz Eberle1, Dieter Schuh1, Benedikt Grünewald1
1Institute for Experimental and Applied Physics, University of Regensburg, D-93040 Regensburg, Germany.
Nano letters
|May 31, 2023
概括
研究人员在非弹性旋转场效应晶体管 (sFET) 中展示了门控制的旋转前置. 这一突破允许在超过电子平均自由路径的距离上保持连贯的自旋旋转,从而使在较不苛刻的材料中实现了自旋电子功能.
科学领域:
- 这就是Spintronics.
- 半导体物理 半导体物理
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 电气控制的旋转旋转对于旋转电子设备,如旋转场效应晶体管 (sFET) 至关重要.
- 之前的电控旋转前行演示主要在弹道模式下运行,需要高旋转轨道合 (SOC) 材料.
- 在非弹道运输系统中实现旋转控制一直是一个重大挑战.
研究的目的:
- 为了证明一个非弹性旋转场效应晶体管 (sFET) 中的门控制的旋转前置.
- 为了证明连贯自旋旋转在远远超过电子平均自由路径的距离上是可能的.
- 放松最初sFET提案中严格的材料要求.
主要方法:
- 使用了旋场效应晶体管 (sFET) 架构,使用一系列狭窄的扩散电线作为通道.
- 采用门控制机制,在半导体通道中诱导旋转前行.
- 在非弹道系统中研究了自旋传输,其中电子散射是显著的.
主要成果:
- 在非弹道式sFET中成功证明了旋转的门控制的前行.
- 在远远超过电子平均自由路径的距离上展示了连贯的自旋旋转.
- 在具有相对较低旋转轨道合 (SOC) 的通道中确认了旋转晶体管功能.
结论:
- 在非弹性半导体通道中,可以实现门控制的旋转前行.
- 这种方法减轻了对高SOC材料的需求,并扩大了旋转电子设备的操作距离.
- 这些发现为在不那么严格的条件下实现实际的自旋电子设备铺平了道路.
相关概念视频
Atomic Nuclei: Nuclear Relaxation Processes
686
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.
686
Atomic Nuclei: Nuclear Spin State Overview
1.0K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
1.0K
Atomic Nuclei: Nuclear Spin
2.1K
All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not...
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not...
2.1K
Atomic Nuclei: Nuclear Spin State Population Distribution
1.0K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
1.0K
Atomic Nuclei: Magnetic Resonance
696
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...
696
Atomic Nuclei: Nuclear Magnetic Moment
1.2K
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...
1.2K


