Bistability in Semiconductor Lasers With Polarization-Rotated Frequency-Dependent Optical Feedback
Bistability in the emission frequency of a semiconductor laser subject to orthogonal-polarization optical feedback was recently observed experimentally by Farias in 2005, Phys. Rev. Lett. 94 173902 (2005). A frequency-sensitive filter (Cs-vapor cell) was placed in the way of the feedback beam to spe...
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description | Bistability in the emission frequency of a semiconductor laser subject to orthogonal-polarization optical feedback was recently observed experimentally by Farias in 2005, Phys. Rev. Lett. 94 173902 (2005). A frequency-sensitive filter (Cs-vapor cell) was placed in the way of the feedback beam to spectrally modulate the feedback power. Two different emission frequencies with the same output power were observed. This observation was understood in terms of a model that took into account the line shape of the filter and the empirical linear relation between the feedback-induced frequency shift and the feedback intensity. The model allowed to calculate steady states but not time-varying solutions. Here we present a rate-equation model that takes into account thermal and gain-saturation effects, and predicts a linear variation of the laser frequency with the feedback strength, together with a small power modulation. This model allows to study time-dependent solutions, and in particular, the transition between the two coexisting states. We show that numerical simulations using this model correctly reproduce the previous observed dynamics, and we present new experimental results in good agreement with our model for the laser response under orthogonal feedback |
doi_str_mv | 10.1109/JQE.2006.889647 |
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Rev. Lett. 94 173902 (2005). A frequency-sensitive filter (Cs-vapor cell) was placed in the way of the feedback beam to spectrally modulate the feedback power. Two different emission frequencies with the same output power were observed. This observation was understood in terms of a model that took into account the line shape of the filter and the empirical linear relation between the feedback-induced frequency shift and the feedback intensity. The model allowed to calculate steady states but not time-varying solutions. Here we present a rate-equation model that takes into account thermal and gain-saturation effects, and predicts a linear variation of the laser frequency with the feedback strength, together with a small power modulation. This model allows to study time-dependent solutions, and in particular, the transition between the two coexisting states. We show that numerical simulations using this model correctly reproduce the previous observed dynamics, and we present new experimental results in good agreement with our model for the laser response under orthogonal feedback</description><identifier>ISSN: 0018-9197</identifier><identifier>EISSN: 1558-1713</identifier><identifier>DOI: 10.1109/JQE.2006.889647</identifier><identifier>CODEN: IEJQA7</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Beams (radiation) ; Bistability ; Chirp modulation ; Emission ; Exact sciences and technology ; Feedback ; Frequency ; Fundamental areas of phenomenology (including applications) ; Laser beams ; Laser feedback ; Laser modes ; Laser transitions ; Lasers ; Mathematical models ; Nonlinear optics ; Optical bistability, multistability and switching, including local field effects ; Optical feedback ; Optical filters ; Optical polarization ; Optics ; Physics ; Semiconductor lasers ; Semiconductor lasers; laser diodes ; Studies</subject><ispartof>IEEE journal of quantum electronics, 2007-03, Vol.43 (3), p.261-268</ispartof><rights>2007 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2007</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c455t-45e3f3307f28d4a42104e6bd63f3946152474a89ec304745763aa9db66e7f4483</citedby><cites>FETCH-LOGICAL-c455t-45e3f3307f28d4a42104e6bd63f3946152474a89ec304745763aa9db66e7f4483</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/4089104$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27922,27923,54756</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/4089104$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=18654854$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Masoller, C.</creatorcontrib><creatorcontrib>Sorrentino, T.</creatorcontrib><creatorcontrib>Chevrollier, M.</creatorcontrib><creatorcontrib>Oria, M.</creatorcontrib><title>Bistability in Semiconductor Lasers With Polarization-Rotated Frequency-Dependent Optical Feedback</title><title>IEEE journal of quantum electronics</title><addtitle>JQE</addtitle><description>Bistability in the emission frequency of a semiconductor laser subject to orthogonal-polarization optical feedback was recently observed experimentally by Farias in 2005, Phys. Rev. Lett. 94 173902 (2005). A frequency-sensitive filter (Cs-vapor cell) was placed in the way of the feedback beam to spectrally modulate the feedback power. Two different emission frequencies with the same output power were observed. This observation was understood in terms of a model that took into account the line shape of the filter and the empirical linear relation between the feedback-induced frequency shift and the feedback intensity. The model allowed to calculate steady states but not time-varying solutions. Here we present a rate-equation model that takes into account thermal and gain-saturation effects, and predicts a linear variation of the laser frequency with the feedback strength, together with a small power modulation. This model allows to study time-dependent solutions, and in particular, the transition between the two coexisting states. We show that numerical simulations using this model correctly reproduce the previous observed dynamics, and we present new experimental results in good agreement with our model for the laser response under orthogonal feedback</description><subject>Beams (radiation)</subject><subject>Bistability</subject><subject>Chirp modulation</subject><subject>Emission</subject><subject>Exact sciences and technology</subject><subject>Feedback</subject><subject>Frequency</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Laser beams</subject><subject>Laser feedback</subject><subject>Laser modes</subject><subject>Laser transitions</subject><subject>Lasers</subject><subject>Mathematical models</subject><subject>Nonlinear optics</subject><subject>Optical bistability, multistability and switching, including local field effects</subject><subject>Optical feedback</subject><subject>Optical filters</subject><subject>Optical polarization</subject><subject>Optics</subject><subject>Physics</subject><subject>Semiconductor lasers</subject><subject>Semiconductor lasers; laser diodes</subject><subject>Studies</subject><issn>0018-9197</issn><issn>1558-1713</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNp9kUFvEzEQhS1EJULLuQcuKyRKL5va67HXPtLStKBIBdqK48rrnRUuGzvYziH8ehylKhKHnmyPv3maeY-QY0bnjFF99uXb5byhVM6V0hLaF2TGhFA1axl_SWaUMlVrpttX5HVKD-UJoOiM9OcuZdO7yeVt5Xx1iytngx82NodYLU3CmKofLv-svobJRPfHZBd8_T1kk3GoFhF_b9Dbbf0J1-gH9Lm6WWdnzVQtEIfe2F9H5GA0U8I3j-chuV9c3l1c18ubq88XH5e1BSFyDQL5yDltx0YNYKBhFFD2gyxVDZKJBlowSqPltNxEK7kxeuilxHYsy_BD8mGvu46hDJVyt3LJ4jQZj2GTOk25bIoqK-TJsyQHYFJxWsDTZ0FGOWu0UkIU9N1_6EPYRF8W7pQE2jQt3UFne8jGkFLEsVtHtzJxW5S6XYpdSbHbpdjtUywd7x9lTSqmjtF469K_NiUFKAGFe7vnHCI-fQNVutjI_wKlGaOm</recordid><startdate>20070301</startdate><enddate>20070301</enddate><creator>Masoller, C.</creator><creator>Sorrentino, T.</creator><creator>Chevrollier, M.</creator><creator>Oria, M.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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Rev. Lett. 94 173902 (2005). A frequency-sensitive filter (Cs-vapor cell) was placed in the way of the feedback beam to spectrally modulate the feedback power. Two different emission frequencies with the same output power were observed. This observation was understood in terms of a model that took into account the line shape of the filter and the empirical linear relation between the feedback-induced frequency shift and the feedback intensity. The model allowed to calculate steady states but not time-varying solutions. Here we present a rate-equation model that takes into account thermal and gain-saturation effects, and predicts a linear variation of the laser frequency with the feedback strength, together with a small power modulation. This model allows to study time-dependent solutions, and in particular, the transition between the two coexisting states. We show that numerical simulations using this model correctly reproduce the previous observed dynamics, and we present new experimental results in good agreement with our model for the laser response under orthogonal feedback</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/JQE.2006.889647</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Beams (radiation) Bistability Chirp modulation Emission Exact sciences and technology Feedback Frequency Fundamental areas of phenomenology (including applications) Laser beams Laser feedback Laser modes Laser transitions Lasers Mathematical models Nonlinear optics Optical bistability, multistability and switching, including local field effects Optical feedback Optical filters Optical polarization Optics Physics Semiconductor lasers Semiconductor lasers laser diodes Studies |
title | Bistability in Semiconductor Lasers With Polarization-Rotated Frequency-Dependent Optical Feedback |
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