†Institute of Solid State Physics, Friedrich-Schiller-University Jena, Max-Wien-Platz 1, 07743 Jena, Germany.
‡Imperial College London, Prince Consort Road, SW7 2BZ London, United Kingdom.
Nano Lett. 2015 Jul 8;15(7):4637-43. doi: 10.1021/acs.nanolett.5b01271. Epub 2015 Jun 24.
Semiconductor nanowire lasers operate at ultrafast timescales; here we report their temporal dynamics, including laser onset time and pulse width, using a double-pump approach. Wide bandgap gallium nitride (GaN), zinc oxide (ZnO), and cadmium sulfide (CdS) nanowires reveal laser onset times of a few picoseconds, driven by carrier thermalization within the optically excited semiconductor. Strong carrier-phonon coupling in ZnO leads to the fastest laser onset time of ∼1 ps in comparison to CdS and GaN exhibiting values of ∼2.5 and ∼3.5 ps, respectively. These values are constant between nanowires of different sizes implying independence from any optical influences. However, we demonstrate that the lasing onset times vary with excitation wavelength relative to the semiconductor band gap. Meanwhile, the laser pulse widths are dependent on the optical system. While the fastest ultrashort pulses are attained using the thinnest possible nanowires, a sudden change in pulse width from ∼5 to ∼15 ps occurs at a critical nanowire diameter. We attribute this to the transition from single to multimode waveguiding, as it is accompanied by a change in laser polarization.
半导体纳米线激光器在超快时间尺度下工作;在这里,我们使用双泵浦方法报告了它们的时间动力学,包括激光起始时间和脉冲宽度。宽带隙氮化镓 (GaN)、氧化锌 (ZnO) 和硫化镉 (CdS) 纳米线在光激发半导体内的载流子热化的驱动下,显示出几皮秒的激光起始时间。在 ZnO 中,强载流子-声子耦合导致最快的激光起始时间约为 1 ps,而 CdS 和 GaN 的相应值分别约为 2.5 和 3.5 ps。这些值在不同尺寸的纳米线之间保持不变,意味着与任何光学影响无关。然而,我们证明激光起始时间随相对于半导体能带隙的激发波长而变化。同时,激光脉冲宽度取决于光学系统。虽然使用尽可能薄的纳米线获得最快的超短脉冲,但在临界纳米线直径处,脉冲宽度会突然从约 5 ps 变化到约 15 ps。我们将其归因于从单模到多模波导的转变,因为它伴随着激光偏振的变化。