Graphene saturable absorber mirror for passive mode-locking of mid-infrared QCLs

被引:0
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作者
A. Outafat
S. Faci
E. Richalot
S. Protat
C. Algani
机构
[1] CNRS,Univ Gustave Eiffel,
[2] CNAM, Univ Gustave Eiffel
[3] ESYCOM,undefined
[4] CNRS,undefined
[5] ESYCOM,undefined
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关键词
Quantum cascade laser; Mode-locked laser; Maxwell-bloch equations; Graphene; Numerical simulation; FDTD;
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摘要
Passive mode-locking in quantum cascade lasers (QCLs) remains one of the huge challenges because of the fast relaxation time of the excited carriers which is typically in the range of sub-picoseconds. The use of conventional techniques such as the semiconductor saturable absorber mirror is inefficient because the spatial hole burning effect dominates the carrier dynamics. To overcome this effect, longitudinal transition structures with relaxation time around 50ps\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$50~\mathrm {ps}$$\end{document} were proposed. However, mode-locking is assured with an external modulation at a cavity roundtrip frequency. In this paper, we demonstrate that a single-layer graphene used as a saturable absorber permits to generate stable pulses in such structures. The graphene is integrated with a highly reflective mirror to increase the internal electric field and achieve the saturation intensity. The dynamic of the QCL is modeled with Maxwell-Bloch equations while Maxwell-Ampere equation is used for the graphene layer by considering a nonlinear conductivity. This system of equations is solved using the one-dimensional Finite-Difference Time-Domain (
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