Kavli Institute of Nanoscience, TU Delft, Lorentzweg 1, 2628 CJ Delft, Netherlands.
RIKEN Center for Emergent Matter Science, Wako-shi, Saitama 351-0198, Japan and Institute of Physics, Slovak Academy of Sciences, Dubravska cesta 9, 84511 Bratislava, Slovakia.
Phys Rev Lett. 2014 Dec 19;113(25):256802. doi: 10.1103/PhysRevLett.113.256802.
We report that the electron spin-relaxation time T_{1} in a GaAs quantum dot with a spin-1/2 ground state has a 180° periodicity in the orientation of the in-plane magnetic field. This periodicity has been predicted for circular dots as being due to the interplay of Rashba and Dresselhaus spin orbit contributions. Different from this prediction, we find that the extrema in the T_{1} do not occur when the magnetic field is along the [110] and [11[over ¯]0] crystallographic directions. This deviation is attributed to an elliptical dot confining potential. The T_{1} varies by more than 1 order of magnitude when rotating a 3 T field, reaching about 80 ms for the optimal angle. We infer from the data that in our device the signs of the Rashba and Dresselhaus constants are opposite.
我们报告称,在具有自旋-1/2基态的 GaAs 量子点中,电子自旋弛豫时间 T_{1}在面内磁场的方向上具有 180°周期性。这种周期性已被预测为圆形点,原因是 Rashba 和 Dresselhaus 自旋轨道贡献的相互作用。与这一预测不同的是,我们发现当磁场沿[110]和[11[over ¯]0]晶向时,T_{1}的极值不会出现。这种偏差归因于椭圆量子点限制势。当旋转 3 T 场时,T_{1}变化超过 1 个数量级,在最佳角度下达到约 80 ms。我们从数据中推断出,在我们的器件中,Rashba 和 Dresselhaus 常数的符号是相反的。