Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum Well

GaInNAs has been introduced to design an active switch operating at wavelength <formula formulatype="inline"> <tex Notation="TeX">$\lambda = 1.2855\ \mu\hbox{m}$</tex></formula> having high selectivity. The device is made of a mono-dimensional periodic pho...

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Main Authors: Giovanna Calo, Dimitris Alexandropoulos, Vincenzo Petruzzelli
Format: Article
Language:English
Published: IEEE 2012-01-01
Series:IEEE Photonics Journal
Subjects:
Online Access:https://ieeexplore.ieee.org/document/6322997/
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author Giovanna Calo
Dimitris Alexandropoulos
Vincenzo Petruzzelli
author_facet Giovanna Calo
Dimitris Alexandropoulos
Vincenzo Petruzzelli
author_sort Giovanna Calo
collection DOAJ
description GaInNAs has been introduced to design an active switch operating at wavelength <formula formulatype="inline"> <tex Notation="TeX">$\lambda = 1.2855\ \mu\hbox{m}$</tex></formula> having high selectivity. The device is made of a mono-dimensional periodic photonic band-gap structure constituted by alternating ridge waveguide layers with different ridge heights. The periodic waveguiding structure has been designed to show the band gap in correspondence of the wavelength range where the dilute nitride active material experiences maximum gain. As an example, the performances of the switch under electrical control are crosstalk <formula formulatype="inline"><tex Notation="TeX">$\hbox{CT} = -14.1\ \hbox{dB}$</tex></formula>, gain in the on-state <formula formulatype="inline"><tex Notation="TeX">${\rm G} = 7.6\ \hbox{dB}$</tex></formula>, and bandwidth <formula formulatype="inline"><tex Notation="TeX">$\Delta\lambda_{-10\,{\rm dB}} = 1.5\ \hbox{nm}$</tex></formula>. By increasing the input power above the optical threshold value of the gain saturation, the switching performance worsens in terms of crosstalk and gain, but the wavelength selectivity improves, since the bandwidth decreases down to <formula formulatype="inline"><tex Notation="TeX">$\Delta\lambda_{-10\,{\rm dB}} = 0.8\ \hbox{nm}$</tex></formula> for the input optical power <formula formulatype="inline"><tex Notation="TeX">${\rm P}_{i} = 20\ \hbox{mW}$</tex></formula>.
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spelling doaj.art-fb542881596e400f8a1e79ffd129b26c2022-12-21T23:01:50ZengIEEEIEEE Photonics Journal1943-06552012-01-01451936194610.1109/JPHOT.2012.22201286322997Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum WellGiovanna Calo0Dimitris Alexandropoulos1Vincenzo Petruzzelli2<formula formulatype="inline"><tex Notation="TeX">$^{1}$</tex></formula>Dipartimento di Elettrotecnica ed Elettronica, Politecnico di Bari, Bari, Italy<formula formulatype="inline"><tex Notation="TeX">$^{2}$</tex></formula> Department of Materials Science, University of Patras, Patras, GreeceDipartimento di Elettrotecnica ed Elettronica, Politecnico di Bari , Bari, ItalyGaInNAs has been introduced to design an active switch operating at wavelength <formula formulatype="inline"> <tex Notation="TeX">$\lambda = 1.2855\ \mu\hbox{m}$</tex></formula> having high selectivity. The device is made of a mono-dimensional periodic photonic band-gap structure constituted by alternating ridge waveguide layers with different ridge heights. The periodic waveguiding structure has been designed to show the band gap in correspondence of the wavelength range where the dilute nitride active material experiences maximum gain. As an example, the performances of the switch under electrical control are crosstalk <formula formulatype="inline"><tex Notation="TeX">$\hbox{CT} = -14.1\ \hbox{dB}$</tex></formula>, gain in the on-state <formula formulatype="inline"><tex Notation="TeX">${\rm G} = 7.6\ \hbox{dB}$</tex></formula>, and bandwidth <formula formulatype="inline"><tex Notation="TeX">$\Delta\lambda_{-10\,{\rm dB}} = 1.5\ \hbox{nm}$</tex></formula>. By increasing the input power above the optical threshold value of the gain saturation, the switching performance worsens in terms of crosstalk and gain, but the wavelength selectivity improves, since the bandwidth decreases down to <formula formulatype="inline"><tex Notation="TeX">$\Delta\lambda_{-10\,{\rm dB}} = 0.8\ \hbox{nm}$</tex></formula> for the input optical power <formula formulatype="inline"><tex Notation="TeX">${\rm P}_{i} = 20\ \hbox{mW}$</tex></formula>.https://ieeexplore.ieee.org/document/6322997/Photonic crystals, quantum well devices, semiconductor materials, optical switches
spellingShingle Giovanna Calo
Dimitris Alexandropoulos
Vincenzo Petruzzelli
Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum Well
IEEE Photonics Journal
Photonic crystals, quantum well devices, semiconductor materials, optical switches
title Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum Well
title_full Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum Well
title_fullStr Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum Well
title_full_unstemmed Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum Well
title_short Active Photonic Band-Gap Switch Based on GaInNAs Multiquantum Well
title_sort active photonic band gap switch based on gainnas multiquantum well
topic Photonic crystals, quantum well devices, semiconductor materials, optical switches
url https://ieeexplore.ieee.org/document/6322997/
work_keys_str_mv AT giovannacalo activephotonicbandgapswitchbasedongainnasmultiquantumwell
AT dimitrisalexandropoulos activephotonicbandgapswitchbasedongainnasmultiquantumwell
AT vincenzopetruzzelli activephotonicbandgapswitchbasedongainnasmultiquantumwell