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具有InAs/InGaAs量子点的微盘激光器中双态激光的温度演化

Temperature Evolution of Two-State Lasing in Microdisk Lasers with InAs/InGaAs Quantum Dots.

作者信息

Makhov Ivan, Ivanov Konstantin, Moiseev Eduard, Fominykh Nikita, Dragunova Anna, Kryzhanovskaya Natalia, Zhukov Alexey

机构信息

International Laboratory of Quantum Optoelectronics, HSE University, Soyuza Pechatnikov Str., 16, St. Petersburg 190008, Russia.

出版信息

Nanomaterials (Basel). 2023 Feb 26;13(5):877. doi: 10.3390/nano13050877.

Abstract

One-state and two-state lasing is investigated experimentally and through numerical simulation as a function of temperature in microdisk lasers with Stranski-Krastanow InAs/InGaAs/GaAs quantum dots. Near room temperature, the temperature-induced increment of the ground-state threshold current density is relatively weak and can be described by a characteristic temperature of about 150 K. At elevated temperatures, a faster (super-exponential) increase in the threshold current density is observed. Meanwhile, the current density corresponding to the onset of two-state lasing was found to decrease with increasing temperature, so that the interval of current density of pure one-state lasing becomes narrower with the temperature increase. Above a certain critical temperature, ground-state lasing completely disappears. This critical temperature drops from 107 to 37 °C as the microdisk diameter decreases from 28 to 20 μm. In microdisks with a diameter of 9 μm, a temperature-induced jump in the lasing wavelength from the first excited-state to second excited-state optical transition is observed. A model describing the system of rate equations and free carrier absorption dependent on the reservoir population provides a satisfactory agreement with experimental results. The temperature and threshold current corresponding to the quenching of ground-state lasing can be well approximated by linear functions of saturated gain and output loss.

摘要

在具有应变层自组装InAs/InGaAs/GaAs量子点的微盘激光器中,通过实验和数值模拟研究了单态和双态激光作为温度的函数。在室温附近,基态阈值电流密度的温度诱导增量相对较弱,可用约150 K的特征温度来描述。在高温下,观察到阈值电流密度有更快(超指数)的增加。同时,发现对应双态激光起始的电流密度随温度升高而降低,因此纯单态激光的电流密度区间随温度升高而变窄。高于某个临界温度,基态激光完全消失。当微盘直径从28μm减小到20μm时,该临界温度从107℃降至37℃。在直径为9μm的微盘中,观察到激光波长从第一激发态到第二激发态光学跃迁的温度诱导跃变。一个描述速率方程组和依赖于载流子库数量的自由载流子吸收的模型与实验结果吻合良好。对应基态激光猝灭的温度和阈值电流可用饱和增益和输出损耗的线性函数很好地近似。

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