Dual-Comb Generation in III-V Semiconductor Laser: Transverse Modes Versus Modeless Cavities

Dual frequency-combs have been relevant for applications such as spectroscopy [1], Many methods are used to generate dual-combs like polarization multiplexing [2] or wavelength/space multiplexing [3], [4]. We demonstrated two passively mode-locked dual-comb configurations in a single Vertical External-Cavity Surface-Emitting Laser (VECSEL) using a InGaAs/GaAs based optically-pumped gain mirror (1/2-VCSEL) and a fast Semiconductor Saturable Absorber Mirror (SESAM) for an emission at <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$1.06\mu \mathrm{m}$</tex> with a pulse width of 5ps at 1GHz repetition rate. Fig. 1 a) shows the cavity design where two lenses are used to control the beam ratio on the gain mirror and the SESAM for a stable mode-locking state, <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$f_{1,2}$</tex> and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$d_{1,2,3}$</tex> are chosen in order to get a stable Laguerre-Gauss (LG) transverse modes oscillations with one optical axis and two transverse states as shown in Fig. 1 b) (up), or a modeless self-imaging cavity with two optical axes as shown in Fig. 1 b) (down). Fig. 1 c) shows the temporal evolution of the dual-comb where the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{LG}_{00}$</tex> comb's repetition rate is <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$f_{rep}=1/T$</tex> and the LG03 comb's one is <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$f_{rep}+\Delta f$</tex> where <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$T$</tex> is the roundtrip time of 1 ns and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\Delta f\approx 100\text{kHz}$</tex>.

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Published
2025-06-23
DOI
https://doi.org/10.1109/cleo/europe-eqec65582.2025.11109387
Primary Topic
Advanced Fiber Laser Technologies
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article
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article

Dual-Comb Generation in III-V Semiconductor Laser: Transverse Modes Versus Modeless Cavities

S. Blin, Adrián Bartolo, Konstantinos Pantzas, L. Le Gratiet et al.
Advanced Fiber Laser Technologies
article

Dual-Comb Generation in III-V Semiconductor Laser: Transverse Modes Versus Modeless Cavities

S. Blin, Adrián Bartolo, Konstantinos Pantzas, L. Le Gratiet, I. Sagnes, Baptiste Chomet, F. González‐Posada, Mohamed Nadrani, Arnaud Garnache, Nathan Vigne, G. Beaudoin
article en

Abstract

Dual frequency-combs have been relevant for applications such as spectroscopy [1], Many methods are used to generate dual-combs like polarization multiplexing [2] or wavelength/space multiplexing [3], [4]. We demonstrated two passively mode-locked dual-comb configurations in a single Vertical External-Cavity Surface-Emitting Laser (VECSEL) using a InGaAs/GaAs based optically-pumped gain mirror (1/2-VCSEL) and a fast Semiconductor Saturable Absorber Mirror (SESAM) for an emission at <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$1.06\mu \mathrm{m}$</tex> with a pulse width of 5ps at 1GHz repetition rate. Fig. 1 a) shows the cavity design where two lenses are used to control the beam ratio on the gain mirror and the SESAM for a stable mode-locking state, <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$f_{1,2}$</tex> and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$d_{1,2,3}$</tex> are chosen in order to get a stable Laguerre-Gauss (LG) transverse modes oscillations with one optical axis and two transverse states as shown in Fig. 1 b) (up), or a modeless self-imaging cavity with two optical axes as shown in Fig. 1 b) (down). Fig. 1 c) shows the temporal evolution of the dual-comb where the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\text{LG}_{00}$</tex> comb's repetition rate is <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$f_{rep}=1/T$</tex> and the LG03 comb's one is <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$f_{rep}+\Delta f$</tex> where <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$T$</tex> is the roundtrip time of 1 ns and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\Delta f\approx 100\text{kHz}$</tex>.

Centre National de la Recherche Scientifique (FR), Université de Montpellier (FR), Centre de Nanosciences et de Nanotechnologies (FR), Institut d'Électronique et des Systèmes (FR)
European Regional Development Fund
Affordable and clean energy
Openalex Percentile: Top 83%
Advanced Fiber Laser Technologies
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