Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation
Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (7...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bello-Jiménez, M. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2011 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer-Verlag 2011 |
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| Übergeordnetes Werk: |
Enthalten in: Applied physics - Berlin : Springer, 1981, 105(2011), 2 vom: 13. Mai, Seite 269-276 |
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| Übergeordnetes Werk: |
volume:105 ; year:2011 ; number:2 ; day:13 ; month:05 ; pages:269-276 |
| Links: |
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| DOI / URN: |
10.1007/s00340-011-4548-6 |
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| Katalog-ID: |
SPR004237129 |
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| 100 | 1 | |a Bello-Jiménez, M. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation |
| 264 | 1 | |c 2011 | |
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| 520 | |a Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. | ||
| 650 | 4 | |a Pump Power |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Wavelength Division Multiplexer |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Modulation Depth |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Ring Laser |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Resonant Wavelength |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Cuadrado-Laborde, C. |4 aut | |
| 700 | 1 | |a Diez, A. |4 aut | |
| 700 | 1 | |a Cruz, J. L. |4 aut | |
| 700 | 1 | |a Andrés, M. V. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Applied physics |d Berlin : Springer, 1981 |g 105(2011), 2 vom: 13. Mai, Seite 269-276 |w (DE-627)253389933 |w (DE-600)1458437-2 |x 1432-0649 |7 nnns |
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10.1007/s00340-011-4548-6 doi (DE-627)SPR004237129 (SPR)s00340-011-4548-6-e DE-627 ger DE-627 rakwb eng Bello-Jiménez, M. verfasserin aut Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2011 Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. Pump Power (dpeaa)DE-He213 Wavelength Division Multiplexer (dpeaa)DE-He213 Modulation Depth (dpeaa)DE-He213 Ring Laser (dpeaa)DE-He213 Resonant Wavelength (dpeaa)DE-He213 Cuadrado-Laborde, C. aut Diez, A. aut Cruz, J. L. aut Andrés, M. V. aut Enthalten in Applied physics Berlin : Springer, 1981 105(2011), 2 vom: 13. Mai, Seite 269-276 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:105 year:2011 number:2 day:13 month:05 pages:269-276 https://dx.doi.org/10.1007/s00340-011-4548-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 105 2011 2 13 05 269-276 |
| spelling |
10.1007/s00340-011-4548-6 doi (DE-627)SPR004237129 (SPR)s00340-011-4548-6-e DE-627 ger DE-627 rakwb eng Bello-Jiménez, M. verfasserin aut Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2011 Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. Pump Power (dpeaa)DE-He213 Wavelength Division Multiplexer (dpeaa)DE-He213 Modulation Depth (dpeaa)DE-He213 Ring Laser (dpeaa)DE-He213 Resonant Wavelength (dpeaa)DE-He213 Cuadrado-Laborde, C. aut Diez, A. aut Cruz, J. L. aut Andrés, M. V. aut Enthalten in Applied physics Berlin : Springer, 1981 105(2011), 2 vom: 13. Mai, Seite 269-276 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:105 year:2011 number:2 day:13 month:05 pages:269-276 https://dx.doi.org/10.1007/s00340-011-4548-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 105 2011 2 13 05 269-276 |
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10.1007/s00340-011-4548-6 doi (DE-627)SPR004237129 (SPR)s00340-011-4548-6-e DE-627 ger DE-627 rakwb eng Bello-Jiménez, M. verfasserin aut Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2011 Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. Pump Power (dpeaa)DE-He213 Wavelength Division Multiplexer (dpeaa)DE-He213 Modulation Depth (dpeaa)DE-He213 Ring Laser (dpeaa)DE-He213 Resonant Wavelength (dpeaa)DE-He213 Cuadrado-Laborde, C. aut Diez, A. aut Cruz, J. L. aut Andrés, M. V. aut Enthalten in Applied physics Berlin : Springer, 1981 105(2011), 2 vom: 13. Mai, Seite 269-276 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:105 year:2011 number:2 day:13 month:05 pages:269-276 https://dx.doi.org/10.1007/s00340-011-4548-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 105 2011 2 13 05 269-276 |
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10.1007/s00340-011-4548-6 doi (DE-627)SPR004237129 (SPR)s00340-011-4548-6-e DE-627 ger DE-627 rakwb eng Bello-Jiménez, M. verfasserin aut Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2011 Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. Pump Power (dpeaa)DE-He213 Wavelength Division Multiplexer (dpeaa)DE-He213 Modulation Depth (dpeaa)DE-He213 Ring Laser (dpeaa)DE-He213 Resonant Wavelength (dpeaa)DE-He213 Cuadrado-Laborde, C. aut Diez, A. aut Cruz, J. L. aut Andrés, M. V. aut Enthalten in Applied physics Berlin : Springer, 1981 105(2011), 2 vom: 13. Mai, Seite 269-276 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:105 year:2011 number:2 day:13 month:05 pages:269-276 https://dx.doi.org/10.1007/s00340-011-4548-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 105 2011 2 13 05 269-276 |
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10.1007/s00340-011-4548-6 doi (DE-627)SPR004237129 (SPR)s00340-011-4548-6-e DE-627 ger DE-627 rakwb eng Bello-Jiménez, M. verfasserin aut Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2011 Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. Pump Power (dpeaa)DE-He213 Wavelength Division Multiplexer (dpeaa)DE-He213 Modulation Depth (dpeaa)DE-He213 Ring Laser (dpeaa)DE-He213 Resonant Wavelength (dpeaa)DE-He213 Cuadrado-Laborde, C. aut Diez, A. aut Cruz, J. L. aut Andrés, M. V. aut Enthalten in Applied physics Berlin : Springer, 1981 105(2011), 2 vom: 13. Mai, Seite 269-276 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:105 year:2011 number:2 day:13 month:05 pages:269-276 https://dx.doi.org/10.1007/s00340-011-4548-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 105 2011 2 13 05 269-276 |
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Enthalten in Applied physics 105(2011), 2 vom: 13. Mai, Seite 269-276 volume:105 year:2011 number:2 day:13 month:05 pages:269-276 |
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Bello-Jiménez, M. @@aut@@ Cuadrado-Laborde, C. @@aut@@ Diez, A. @@aut@@ Cruz, J. L. @@aut@@ Andrés, M. V. @@aut@@ |
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Bello-Jiménez, M. |
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Bello-Jiménez, M. misc Pump Power misc Wavelength Division Multiplexer misc Modulation Depth misc Ring Laser misc Resonant Wavelength Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation |
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Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation Pump Power (dpeaa)DE-He213 Wavelength Division Multiplexer (dpeaa)DE-He213 Modulation Depth (dpeaa)DE-He213 Ring Laser (dpeaa)DE-He213 Resonant Wavelength (dpeaa)DE-He213 |
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Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation |
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Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation |
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Bello-Jiménez, M. |
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Bello-Jiménez, M. |
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experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation |
| title_auth |
Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation |
| abstract |
Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. © Springer-Verlag 2011 |
| abstractGer |
Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. © Springer-Verlag 2011 |
| abstract_unstemmed |
Abstract We report an experimental study of an actively mode-locked fiber ring laser based on the development of an efficient in-fiber amplitude modulator. Intermodal coupling induced by standing flexural acoustic waves permits the implementation of broad bandwidth (1.5 nm), high modulation depth (72%), low-insertion-loss (0.75 dB), in-fiber amplitude modulators, operating in the MHz frequency range. The experimental characterization of the laser as a function of the radio frequency voltage that controls the modulator, the length of the active fiber, and the optical bandwidth of an intracavity filter implemented with a fiber Bragg grating has led to an improved performance of the Erbium-doped fiber laser: optical pulses of 34-ps temporal width, 1.4-W peak power, and 4.75-MHz repetition rate. © Springer-Verlag 2011 |
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Experimental study of an actively mode-locked fiber ring laser based on in-fiber amplitude modulation |
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Cuadrado-Laborde, C. Diez, A. Cruz, J. L. Andrés, M. V. |
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Cuadrado-Laborde, C. Diez, A. Cruz, J. L. Andrés, M. V. |
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| score |
7.400093 |