Deb Swarup, Dhar Subhabrata
Department of Physics, Indian Institute of Technology Bombay, Powai, Mumbai, 400076, India.
Sci Rep. 2021 Mar 5;11(1):5277. doi: 10.1038/s41598-021-84451-y.
A two-dimensional electron gas (2DEG), which has recently been shown to develop in the central vertical plane of a wedge-shaped c-oriented GaN nanowall due to spontaneous polarization effect, offers a unique scenario, where the symmetry between the conduction and valence band is preserved over the entire confining potential. This results in the suppression of Rashba coupling even when the shape of the wedge is not symmetric. Here, for such a 2DEG channel, relaxation time for different spin projections is calculated as a function of donor concentration and gate bias. Our study reveals a strong dependence of the relaxation rate on the spin-orientation and density of carriers in the channel. Most interestingly, relaxation of spin oriented along the direction of confinement has been found to be completely switched off. Upon applying a suitable bias at the gate, the process can be switched on again. Exploiting this fascinating effect, an electrically driven spin-transistor has been proposed.
由于自发极化效应,最近在楔形c取向氮化镓纳米壁的中心垂直平面中已显示出二维电子气(2DEG),它提供了一种独特的情况,即导带和价带之间的对称性在整个限制势中得以保留。这导致即使楔形形状不对称时,Rashba耦合也会受到抑制。在此,对于这样一个二维电子气通道,计算了不同自旋投影的弛豫时间作为施主浓度和栅极偏置的函数。我们的研究揭示了弛豫率强烈依赖于通道中载流子的自旋取向和密度。最有趣的是,已发现沿限制方向取向的自旋弛豫完全被关闭。在栅极施加合适的偏置时,该过程可以再次开启。利用这种引人入胜的效应,已提出了一种电驱动自旋晶体管。