SIST Group Proposes Novel Q-Switched Semiconductor Laser Type

ON2019-06-17TAG: ShanghaiTech UniversityCATEGORY: School of Information Science and Technology

SIST Assistant Professor Wang Cheng’s group proposed a Q-switched quantum-dot semiconductor laser based on a new physical mechanism in a recent issue of the IEEE Journal of Selected Topics in Quantum Electronics, with the title of “Intensity Noise and Pulse Oscillations of an InAs/GaAs Quantum Dot Laser on Germanium.” This laser doesn’t require an absorber section which are required byt conventional Q-switched lasers to include. The laser with a single gain section produces self-sustained pulse oscillations under DC pump current. 

Semiconductor lasers under DC pump usually produce continuous-wave light output. In order to achieve pulsed output, a saturable absorber is required to achieve either Q-switching or mode locking. The group’s work proposes to employ InAs/GaAs quantum dot lasers epitaxially grown on germanium substrate to achieve pulse oscillation, without incorporating any saturable absorber. Through adjusting the DC pump current, the laser produces both period-one and period-two oscillations as shown in Fig. 1. These periodic oscillations are desirable both for nonlinear dynamics field and for photonic microwave applications. The physical mechanism takes advantage of the inhomogeneous broadening nature of the quantum dots. One non-lasing dot group provides saturable absorption for another lasing dot group with energy overlap, and hence leads to self Q-switching pulse oscillation. This new mechanism can significantly simplify the design of pulsed laser sources in photonic integrated circuits on silicon. 

Their work was finished in collaboration with Telecom Paristech, France, and with SIMIT, Chinese Academy of Science. It was financially supported by Natural Science Foundation of China, and by Shanghai Pujiang Program.  

Read more at:https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=8717669

Figure 1. Electrical spectra (left), time series (middle), and phase portraits (right) at different pump currents. (a) and (d) are period-one oscillations, (b) and (c) are period-two oscillations.