Optically coupled cavities for wavelength switching
An optical bistable device which presents hysteresis behavior is proposed and experimentally demonstrated. The system finds applications in wavelength switching, pulse reshaping and optical bistability. It is based on two optically coupled cavities named master and slave. Each cavity includes a semi...
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2011
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Acceso en línea: | http://sedici.unlp.edu.ar/handle/10915/127317 https://iopscience.iop.org/article/10.1088/1742-6596/274/1/012022 |
Aporte de: | SEDICI (UNLP) de Universidad Nacional de La Plata Ver origen |
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I19-R120-10915-1273172021-10-26T20:07:05Z http://sedici.unlp.edu.ar/handle/10915/127317 https://iopscience.iop.org/article/10.1088/1742-6596/274/1/012022 issn:1742-6596 Optically coupled cavities for wavelength switching Costanzo Caso, Pablo Alejandro Granieri, Sergio Siahmakoun, Azad 2011-01-01 2021-10-26T18:10:18Z es Ciencias Exactas Física hysteresis behavior fiber Bragg gratings semiconductor optical amplifier variable optical coupler An optical bistable device which presents hysteresis behavior is proposed and experimentally demonstrated. The system finds applications in wavelength switching, pulse reshaping and optical bistability. It is based on two optically coupled cavities named master and slave. Each cavity includes a semiconductor optical amplifier (SOA), acting as the gain medium of the laser, and two pair of fiber Bragg gratings (FBG) which define the lasing wavelength (being different in each cavity). Finally, a variable optical coupler (VOC) is employed to couple both cavities. Experimental characterization of the system performance is made analyzing the effects of the coupling coefficient between the two cavities and the driving current in each SOA. The properties of the hysteretic bistable curve and switching can be controlled by adjusting these parameters and the loss in the cavities. By selecting the output wavelength (λ<sub>1</sub> or λ<sub>2</sub>) with an external filter it is possible to choose either the invert or non-invert switched signal. Experiments were developed employing both optical discrete components and a photonic integrated circuit. They show that for 8 m-long cavities the maximum switching frequency is about 500 KHz, and for 4 m-long cavities a minimum rise-time about 21 ns was measured. The switching time can be reduced by shortening the cavity lengths and using photonic integrated circuits. Centro de Investigaciones Ópticas Articulo Articulo http://creativecommons.org/licenses/by/4.0/ Creative Commons Attribution 4.0 International (CC BY 4.0) application/pdf |
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Universidad Nacional de La Plata |
institution_str |
I-19 |
repository_str |
R-120 |
collection |
SEDICI (UNLP) |
language |
Español |
topic |
Ciencias Exactas Física hysteresis behavior fiber Bragg gratings semiconductor optical amplifier variable optical coupler |
spellingShingle |
Ciencias Exactas Física hysteresis behavior fiber Bragg gratings semiconductor optical amplifier variable optical coupler Costanzo Caso, Pablo Alejandro Granieri, Sergio Siahmakoun, Azad Optically coupled cavities for wavelength switching |
topic_facet |
Ciencias Exactas Física hysteresis behavior fiber Bragg gratings semiconductor optical amplifier variable optical coupler |
description |
An optical bistable device which presents hysteresis behavior is proposed and experimentally demonstrated. The system finds applications in wavelength switching, pulse reshaping and optical bistability. It is based on two optically coupled cavities named master and slave. Each cavity includes a semiconductor optical amplifier (SOA), acting as the gain medium of the laser, and two pair of fiber Bragg gratings (FBG) which define the lasing wavelength (being different in each cavity). Finally, a variable optical coupler (VOC) is employed to couple both cavities. Experimental characterization of the system performance is made analyzing the effects of the coupling coefficient between the two cavities and the driving current in each SOA. The properties of the hysteretic bistable curve and switching can be controlled by adjusting these parameters and the loss in the cavities. By selecting the output wavelength (λ<sub>1</sub> or λ<sub>2</sub>) with an external filter it is possible to choose either the invert or non-invert switched signal. Experiments were developed employing both optical discrete components and a photonic integrated circuit. They show that for 8 m-long cavities the maximum switching frequency is about 500 KHz, and for 4 m-long cavities a minimum rise-time about 21 ns was measured. The switching time can be reduced by shortening the cavity lengths and using photonic integrated circuits. |
format |
Articulo Articulo |
author |
Costanzo Caso, Pablo Alejandro Granieri, Sergio Siahmakoun, Azad |
author_facet |
Costanzo Caso, Pablo Alejandro Granieri, Sergio Siahmakoun, Azad |
author_sort |
Costanzo Caso, Pablo Alejandro |
title |
Optically coupled cavities for wavelength switching |
title_short |
Optically coupled cavities for wavelength switching |
title_full |
Optically coupled cavities for wavelength switching |
title_fullStr |
Optically coupled cavities for wavelength switching |
title_full_unstemmed |
Optically coupled cavities for wavelength switching |
title_sort |
optically coupled cavities for wavelength switching |
publishDate |
2011 |
url |
http://sedici.unlp.edu.ar/handle/10915/127317 https://iopscience.iop.org/article/10.1088/1742-6596/274/1/012022 |
work_keys_str_mv |
AT costanzocasopabloalejandro opticallycoupledcavitiesforwavelengthswitching AT granierisergio opticallycoupledcavitiesforwavelengthswitching AT siahmakounazad opticallycoupledcavitiesforwavelengthswitching |
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1734874925710180352 |