Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics
We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical sig...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
You, X [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2016 |
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| Schlagwörter: |
Semiconductor optical amplifiers |
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| Übergeordnetes Werk: |
Enthalten in: IEEE photonics technology letters - New York, NY : IEEE, 1989, 28(2016), 8, Seite 919-922 |
|---|---|
| Übergeordnetes Werk: |
volume:28 ; year:2016 ; number:8 ; pages:919-922 |
| Links: |
|---|
| DOI / URN: |
10.1109/LPT.2016.2517650 |
|---|
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OLC1974107825 |
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| 520 | |a We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. | ||
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10.1109/LPT.2016.2517650 doi PQ20160610 (DE-627)OLC1974107825 (DE-599)GBVOLC1974107825 (PRQ)c70f-146cebbec6afe2a93b8ff3c62d24889952173959796777476982f8611ad330fa0 (KEY)0175401720160000028000800919widelycontinuoustunablepspulsetraingenerationbased DE-627 ger DE-627 rakwb eng 620 DNB 33.38 bkl 53.54 bkl You, X verfasserin aut Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. Shape Semiconductor optical amplifiers Timing jitter Optical pulses Optical propagation in nonlinear media Optical pulse generation Correlation optical pulse compression Erbium-doped fiber amplifiers Optical filters Gosset, C oth Gallion, P oth Enthalten in IEEE photonics technology letters New York, NY : IEEE, 1989 28(2016), 8, Seite 919-922 (DE-627)129622567 (DE-600)246805-0 (DE-576)018141765 1041-1135 nnns volume:28 year:2016 number:8 pages:919-922 http://dx.doi.org/10.1109/LPT.2016.2517650 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7381641 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_231 33.38 AVZ 53.54 AVZ AR 28 2016 8 919-922 |
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10.1109/LPT.2016.2517650 doi PQ20160610 (DE-627)OLC1974107825 (DE-599)GBVOLC1974107825 (PRQ)c70f-146cebbec6afe2a93b8ff3c62d24889952173959796777476982f8611ad330fa0 (KEY)0175401720160000028000800919widelycontinuoustunablepspulsetraingenerationbased DE-627 ger DE-627 rakwb eng 620 DNB 33.38 bkl 53.54 bkl You, X verfasserin aut Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. Shape Semiconductor optical amplifiers Timing jitter Optical pulses Optical propagation in nonlinear media Optical pulse generation Correlation optical pulse compression Erbium-doped fiber amplifiers Optical filters Gosset, C oth Gallion, P oth Enthalten in IEEE photonics technology letters New York, NY : IEEE, 1989 28(2016), 8, Seite 919-922 (DE-627)129622567 (DE-600)246805-0 (DE-576)018141765 1041-1135 nnns volume:28 year:2016 number:8 pages:919-922 http://dx.doi.org/10.1109/LPT.2016.2517650 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7381641 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_231 33.38 AVZ 53.54 AVZ AR 28 2016 8 919-922 |
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10.1109/LPT.2016.2517650 doi PQ20160610 (DE-627)OLC1974107825 (DE-599)GBVOLC1974107825 (PRQ)c70f-146cebbec6afe2a93b8ff3c62d24889952173959796777476982f8611ad330fa0 (KEY)0175401720160000028000800919widelycontinuoustunablepspulsetraingenerationbased DE-627 ger DE-627 rakwb eng 620 DNB 33.38 bkl 53.54 bkl You, X verfasserin aut Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. Shape Semiconductor optical amplifiers Timing jitter Optical pulses Optical propagation in nonlinear media Optical pulse generation Correlation optical pulse compression Erbium-doped fiber amplifiers Optical filters Gosset, C oth Gallion, P oth Enthalten in IEEE photonics technology letters New York, NY : IEEE, 1989 28(2016), 8, Seite 919-922 (DE-627)129622567 (DE-600)246805-0 (DE-576)018141765 1041-1135 nnns volume:28 year:2016 number:8 pages:919-922 http://dx.doi.org/10.1109/LPT.2016.2517650 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7381641 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_231 33.38 AVZ 53.54 AVZ AR 28 2016 8 919-922 |
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10.1109/LPT.2016.2517650 doi PQ20160610 (DE-627)OLC1974107825 (DE-599)GBVOLC1974107825 (PRQ)c70f-146cebbec6afe2a93b8ff3c62d24889952173959796777476982f8611ad330fa0 (KEY)0175401720160000028000800919widelycontinuoustunablepspulsetraingenerationbased DE-627 ger DE-627 rakwb eng 620 DNB 33.38 bkl 53.54 bkl You, X verfasserin aut Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. Shape Semiconductor optical amplifiers Timing jitter Optical pulses Optical propagation in nonlinear media Optical pulse generation Correlation optical pulse compression Erbium-doped fiber amplifiers Optical filters Gosset, C oth Gallion, P oth Enthalten in IEEE photonics technology letters New York, NY : IEEE, 1989 28(2016), 8, Seite 919-922 (DE-627)129622567 (DE-600)246805-0 (DE-576)018141765 1041-1135 nnns volume:28 year:2016 number:8 pages:919-922 http://dx.doi.org/10.1109/LPT.2016.2517650 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7381641 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_231 33.38 AVZ 53.54 AVZ AR 28 2016 8 919-922 |
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10.1109/LPT.2016.2517650 doi PQ20160610 (DE-627)OLC1974107825 (DE-599)GBVOLC1974107825 (PRQ)c70f-146cebbec6afe2a93b8ff3c62d24889952173959796777476982f8611ad330fa0 (KEY)0175401720160000028000800919widelycontinuoustunablepspulsetraingenerationbased DE-627 ger DE-627 rakwb eng 620 DNB 33.38 bkl 53.54 bkl You, X verfasserin aut Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. Shape Semiconductor optical amplifiers Timing jitter Optical pulses Optical propagation in nonlinear media Optical pulse generation Correlation optical pulse compression Erbium-doped fiber amplifiers Optical filters Gosset, C oth Gallion, P oth Enthalten in IEEE photonics technology letters New York, NY : IEEE, 1989 28(2016), 8, Seite 919-922 (DE-627)129622567 (DE-600)246805-0 (DE-576)018141765 1041-1135 nnns volume:28 year:2016 number:8 pages:919-922 http://dx.doi.org/10.1109/LPT.2016.2517650 Volltext http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=7381641 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_231 33.38 AVZ 53.54 AVZ AR 28 2016 8 919-922 |
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620 DNB 33.38 bkl 53.54 bkl Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics Shape Semiconductor optical amplifiers Timing jitter Optical pulses Optical propagation in nonlinear media Optical pulse generation Correlation optical pulse compression Erbium-doped fiber amplifiers Optical filters |
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Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics |
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widely continuous tunable ps pulse train generation based on soa nonlinear dynamics |
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Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics |
| abstract |
We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. |
| abstractGer |
We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. |
| abstract_unstemmed |
We propose a simple setup based on nonlinear dynamics in a semiconductor optical amplifier (SOA) and solitonic compression for the generation of stable and tunable repetition rate picosecond (ps) optical pulses. A quantum-well SOA is used to amplify electrical-optic-modulated rectangular optical signal, during which the nonlinear amplification process induces front-edge distortion. Due to the non-zero linewidth enhancement factor, the front-edge distortion can be isolated by the optical filtration of the chirped frequency component, which eventually becomes Gaussian-like pulse train of tens of ps FWHM pulsewidth. Following a stage of solitonic compression and a stage of pedestal suppression, we are able to obtain a train of 1-ps high-quality pulses for which the root mean square timing jitter is <2.5 ps. The repetition rate exhibits a wide continuous tunability from 70 to 790 MHz as well a wide wavelength tunability in the <inline-formula> <tex-math notation="LaTeX">C </tex-math></inline-formula>-band. |
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Widely Continuous Tunable ps Pulse Train Generation Based on SOA Nonlinear Dynamics |
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