Department of Physics, National Taiwan University, Taipei 106, Taiwan.
Nat Nanotechnol. 2014 Oct;9(10):845-50. doi: 10.1038/nnano.2014.195. Epub 2014 Sep 21.
Besides adding a new functionality to conventional lasers, spin-polarized lasers can, potentially, offer lower threshold currents and reach higher emission intensities. However, to achieve spin-polarized lasing emission a material should possess a slow spin relaxation and a high propensity to be injected with spin-polarized currents. These are stringent requirements that, so far, have limited the choice of candidate materials for spin-lasers. Here we show that these requirements can be relaxed by using a new self-polarized spin mechanism. Fe3O4 nanoparticles are coupled to GaN nanorods to form an energy-band structure that induces the selective charge transfer of electrons with opposite spins. In turn, this selection mechanism generates the population imbalance between spin-up and spin-down electrons in the emitter's energy levels without an external bias. Using this principle, we demonstrate laser emission from GaN nanorods with spin polarization up to 28.2% at room temperature under a low magnetic field of 0.35 T. As the spin-selection mechanism relies entirely on the relative energy-band alignment between the iron oxide nanoparticles and the emitter and requires neither optical pumping with circularly polarized light nor electrical pumping with magnetic electrodes, potentially a wide range of semiconductors can be used as spin-nanolasers.
除了为传统激光器增加新功能外,自旋极化激光器还可能提供更低的阈值电流并达到更高的发射强度。然而,为了实现自旋极化激光发射,材料应该具有缓慢的自旋弛豫和高自旋极化电流注入的倾向。这些是严格的要求,迄今为止,限制了候选自旋激光器材料的选择。在这里,我们展示了可以通过使用新的自极化自旋机制来放宽这些要求。Fe3O4 纳米颗粒与 GaN 纳米棒耦合,形成能带结构,诱导具有相反自旋的电子选择性电荷转移。反过来,这种选择机制在没有外部偏置的情况下,在发射器的能级中产生自旋向上和自旋向下电子之间的粒子数不平衡。利用这一原理,我们在室温下低磁场 0.35 T 下,从 GaN 纳米棒中演示了高达 28.2%的自旋极化激光发射。由于自旋选择机制完全依赖于氧化铁纳米颗粒和发射器之间的相对能带排列,既不需要圆偏振光的光学泵浦,也不需要磁电极的电泵浦,因此可以使用广泛的半导体作为自旋纳米激光器。