In this paper, the authors propose an integrated design of an in-plane optically-pumped edge-emitting ridge-waveguide semiconductor laser, without any bulk components. The optical pump radiation is transferred to the active region of the laser through coupling from the adjacent transparent waveguide. The laser device is based on In1-xGaxAsyP1-y/InP heterojunction, with a pump at 1310 nm wavelength and lasing around 1550 nm. The proposed scheme enables optical-to-optical signal control, in place of the current controlled signal in an electrically-biased semiconductor laser. Since the structure doesn’t require any p-n junctions, a high-quality active material with minimum doping can be employed. In order to simulate the steady-state characteristics of an optically-pumped semiconductor laser, the well-established Connelly’s model for semiconductor optical amplifiers (SOAs) is suitably modified. The validity of the model for semiconductor lasers is established by showing that the evolution of simulated longitudinal modes conforms with the prediction of laser theory. For the chosen device parameters, under optimum operating conditions, the threshold pump power is found to be ≈ 70 mW along with a high pump power conversion efficiency (i.e output laser power/input pump power) of 61%. The proposed all-optically pumped semiconductor laser could be in the form of a 2-port fiber pig-tailed integrated optical device, without the need for any bias current.
Published in | American Journal of Optics and Photonics (Volume 10, Issue 2) |
DOI | 10.11648/j.ajop.20221002.11 |
Page(s) | 10-15 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
Copyright |
Copyright © The Author(s), 2022. Published by Science Publishing Group |
Optical Pumping, Semiconductor Lasers, Integrated Optics, Waveguide Coupling
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APA Style
Nithin Vogirala, Mangalpady Rajaram Shenoy. (2022). Optically-Pumped Edge-Emitting Semiconductor Laser Using Coupled Ridge-Waveguide Structure. American Journal of Optics and Photonics, 10(2), 10-15. https://doi.org/10.11648/j.ajop.20221002.11
ACS Style
Nithin Vogirala; Mangalpady Rajaram Shenoy. Optically-Pumped Edge-Emitting Semiconductor Laser Using Coupled Ridge-Waveguide Structure. Am. J. Opt. Photonics 2022, 10(2), 10-15. doi: 10.11648/j.ajop.20221002.11
@article{10.11648/j.ajop.20221002.11, author = {Nithin Vogirala and Mangalpady Rajaram Shenoy}, title = {Optically-Pumped Edge-Emitting Semiconductor Laser Using Coupled Ridge-Waveguide Structure}, journal = {American Journal of Optics and Photonics}, volume = {10}, number = {2}, pages = {10-15}, doi = {10.11648/j.ajop.20221002.11}, url = {https://doi.org/10.11648/j.ajop.20221002.11}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajop.20221002.11}, abstract = {In this paper, the authors propose an integrated design of an in-plane optically-pumped edge-emitting ridge-waveguide semiconductor laser, without any bulk components. The optical pump radiation is transferred to the active region of the laser through coupling from the adjacent transparent waveguide. The laser device is based on In1-xGaxAsyP1-y/InP heterojunction, with a pump at 1310 nm wavelength and lasing around 1550 nm. The proposed scheme enables optical-to-optical signal control, in place of the current controlled signal in an electrically-biased semiconductor laser. Since the structure doesn’t require any p-n junctions, a high-quality active material with minimum doping can be employed. In order to simulate the steady-state characteristics of an optically-pumped semiconductor laser, the well-established Connelly’s model for semiconductor optical amplifiers (SOAs) is suitably modified. The validity of the model for semiconductor lasers is established by showing that the evolution of simulated longitudinal modes conforms with the prediction of laser theory. For the chosen device parameters, under optimum operating conditions, the threshold pump power is found to be ≈ 70 mW along with a high pump power conversion efficiency (i.e output laser power/input pump power) of 61%. The proposed all-optically pumped semiconductor laser could be in the form of a 2-port fiber pig-tailed integrated optical device, without the need for any bias current.}, year = {2022} }
TY - JOUR T1 - Optically-Pumped Edge-Emitting Semiconductor Laser Using Coupled Ridge-Waveguide Structure AU - Nithin Vogirala AU - Mangalpady Rajaram Shenoy Y1 - 2022/11/04 PY - 2022 N1 - https://doi.org/10.11648/j.ajop.20221002.11 DO - 10.11648/j.ajop.20221002.11 T2 - American Journal of Optics and Photonics JF - American Journal of Optics and Photonics JO - American Journal of Optics and Photonics SP - 10 EP - 15 PB - Science Publishing Group SN - 2330-8494 UR - https://doi.org/10.11648/j.ajop.20221002.11 AB - In this paper, the authors propose an integrated design of an in-plane optically-pumped edge-emitting ridge-waveguide semiconductor laser, without any bulk components. The optical pump radiation is transferred to the active region of the laser through coupling from the adjacent transparent waveguide. The laser device is based on In1-xGaxAsyP1-y/InP heterojunction, with a pump at 1310 nm wavelength and lasing around 1550 nm. The proposed scheme enables optical-to-optical signal control, in place of the current controlled signal in an electrically-biased semiconductor laser. Since the structure doesn’t require any p-n junctions, a high-quality active material with minimum doping can be employed. In order to simulate the steady-state characteristics of an optically-pumped semiconductor laser, the well-established Connelly’s model for semiconductor optical amplifiers (SOAs) is suitably modified. The validity of the model for semiconductor lasers is established by showing that the evolution of simulated longitudinal modes conforms with the prediction of laser theory. For the chosen device parameters, under optimum operating conditions, the threshold pump power is found to be ≈ 70 mW along with a high pump power conversion efficiency (i.e output laser power/input pump power) of 61%. The proposed all-optically pumped semiconductor laser could be in the form of a 2-port fiber pig-tailed integrated optical device, without the need for any bias current. VL - 10 IS - 2 ER -