Wavelength-Stabilized Multi-Active Region DBR and DFB Broad-Area and Ridge-Waveguide Lasers for High Peak-Power Pulsed Operation

For LiDAR applications, compact, robust, and mass-producible light sources generating high-peak power nanosecond-long pulses are essential. This paper presents an investigation of power scaling in semiconductor lasers via the number of epitaxially stacked active regions in a single vertical waveguide supporting a higher order mode, chip length, output aperture width, and lateral waveguide design. All devices are wavelength-stabilized using surface gratings integrated either as a passive section at the rear facet of the diode laser as a distributed-Bragg-reflector (DBR) or along the full length of the chip in a distributed feedback (DFB) design. A 4 mm long broad-area (BA) DBR laser with a stripe width of 200 μm and five active regions delivered approximately 171 W at 80 A, a factor of 6.6 more peak pulse power than the standard 6 mm long single active region DBR laser with 50 μm stripe width. A corresponding 3 mm long 3-active region DFB-BA laser achieved more than 125 W at 129 A. These BA lasers have a lateral beam propagation ratio M<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{2}\approx$</tex-math></inline-formula> 30. In contrast, weakly tapered ridge waveguide (TRW) lasers were found to generate more than 20 W with an M<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{2}$</tex-math></inline-formula> of about 3 and an excellent lateral brightness of 24 W<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\cdot$</tex-math></inline-formula> mm<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{-1}$</tex-math></inline-formula>mrad<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{-1}$</tex-math></inline-formula>.

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Publication Details

Journal
IEEE Journal of Selected Topics in Quantum Electronics
Published
2024-09-03
DOI
https://doi.org/10.1109/jstqe.2024.3454353
Citations
5
Primary Topic
Laser Design and Applications
Type
article
Field-Weighted Citation Impact
1.04

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article

Wavelength-Stabilized Multi-Active Region DBR and DFB Broad-Area and Ridge-Waveguide Lasers for High Peak-Power Pulsed Operation

Nor Ammouri, A. Maaßdorf, A. Ginolas, J. Fricke et al.
5 citations
IEEE Journal of Selected Topics in Quantum Electronics
Laser Design and Applications
1.04
article

Wavelength-Stabilized Multi-Active Region DBR and DFB Broad-Area and Ridge-Waveguide Lasers for High Peak-Power Pulsed Operation

Nor Ammouri, A. Maaßdorf, A. Ginolas, J. Fricke, Jan‐Philipp Koester, H. Wenzel, Andrea Knigge, Armin Liero, Heike Christopher, Maximilian Beier, Sonja Nozinic
article en
5 citations

Abstract

For LiDAR applications, compact, robust, and mass-producible light sources generating high-peak power nanosecond-long pulses are essential. This paper presents an investigation of power scaling in semiconductor lasers via the number of epitaxially stacked active regions in a single vertical waveguide supporting a higher order mode, chip length, output aperture width, and lateral waveguide design. All devices are wavelength-stabilized using surface gratings integrated either as a passive section at the rear facet of the diode laser as a distributed-Bragg-reflector (DBR) or along the full length of the chip in a distributed feedback (DFB) design. A 4 mm long broad-area (BA) DBR laser with a stripe width of 200 μm and five active regions delivered approximately 171 W at 80 A, a factor of 6.6 more peak pulse power than the standard 6 mm long single active region DBR laser with 50 μm stripe width. A corresponding 3 mm long 3-active region DFB-BA laser achieved more than 125 W at 129 A. These BA lasers have a lateral beam propagation ratio M<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{2}\approx$</tex-math></inline-formula> 30. In contrast, weakly tapered ridge waveguide (TRW) lasers were found to generate more than 20 W with an M<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{2}$</tex-math></inline-formula> of about 3 and an excellent lateral brightness of 24 W<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\cdot$</tex-math></inline-formula> mm<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{-1}$</tex-math></inline-formula>mrad<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$^{-1}$</tex-math></inline-formula>.

IEEE Journal of Selected Topics in Quantum ElectronicsVol. 31(2: Pwr. and Effic. Scaling in)
Ferdinand-Braun-Institut (DE)
Deutsches Zentrum für Luft- und Raumfahrt, Forschungsfabrik Mikroelektronik Deutschland
Climate action
Openalex Percentile: Top 23%
Laser Design and Applications
1.04
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