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>.
Authors
- S. Blin (ORCID: https://orcid.org/0000-0003-4339-6861)
- Adrián Bartolo
- Konstantinos Pantzas (ORCID: https://orcid.org/0000-0002-2297-3247)
- L. Le Gratiet
- I. Sagnes (ORCID: https://orcid.org/0000-0001-8068-6599)
- Baptiste Chomet
- F. González‐Posada (ORCID: https://orcid.org/0000-0002-5601-487X)
- Mohamed Nadrani
- Arnaud Garnache
- Nathan Vigne
- G. Beaudoin (ORCID: https://orcid.org/0000-0001-8283-2609)
Institutions
- 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)
Publication Details
- Published
- 2025-06-23
- DOI
- https://doi.org/10.1109/cleo/europe-eqec65582.2025.11109387
- Primary Topic
- Advanced Fiber Laser Technologies
- Type
- article
- Field-Weighted Citation Impact
- 0.00
Funders
- European Regional Development Fund