Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations
Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics o...
Ausführliche Beschreibung
Autor*in: |
Liu, M. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2012 |
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Anmerkung: |
© Pleiades Publishing, Ltd. 2012 |
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Übergeordnetes Werk: |
Enthalten in: Laser physics - Bristol [u.a.] : IOP Publ., 2006, 22(2012), 8 vom: 09. Juli, Seite 1335-1339 |
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Übergeordnetes Werk: |
volume:22 ; year:2012 ; number:8 ; day:09 ; month:07 ; pages:1335-1339 |
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DOI / URN: |
10.1134/S1054660X12080130 |
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SPR020141335 |
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700 | 1 | |a Meng, K. |4 aut | |
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10.1134/S1054660X12080130 doi (DE-627)SPR020141335 (SPR)S1054660X12080130-e DE-627 ger DE-627 rakwb eng Liu, M. verfasserin aut Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. Fiber Laser (dpeaa)DE-He213 Laser Physics (dpeaa)DE-He213 Slow Motion (dpeaa)DE-He213 Pulse Pump (dpeaa)DE-He213 Quiet Period (dpeaa)DE-He213 Zhang, H. T. aut Yan, P. aut Gong, M. L. aut Zheng, C. aut Meng, K. aut Enthalten in Laser physics Bristol [u.a.] : IOP Publ., 2006 22(2012), 8 vom: 09. Juli, Seite 1335-1339 (DE-627)509758444 (DE-600)2228434-5 1555-6611 nnns volume:22 year:2012 number:8 day:09 month:07 pages:1335-1339 https://dx.doi.org/10.1134/S1054660X12080130 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_24 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_110 GBV_ILN_150 GBV_ILN_161 GBV_ILN_213 GBV_ILN_230 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2190 AR 22 2012 8 09 07 1335-1339 |
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10.1134/S1054660X12080130 doi (DE-627)SPR020141335 (SPR)S1054660X12080130-e DE-627 ger DE-627 rakwb eng Liu, M. verfasserin aut Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. Fiber Laser (dpeaa)DE-He213 Laser Physics (dpeaa)DE-He213 Slow Motion (dpeaa)DE-He213 Pulse Pump (dpeaa)DE-He213 Quiet Period (dpeaa)DE-He213 Zhang, H. T. aut Yan, P. aut Gong, M. L. aut Zheng, C. aut Meng, K. aut Enthalten in Laser physics Bristol [u.a.] : IOP Publ., 2006 22(2012), 8 vom: 09. Juli, Seite 1335-1339 (DE-627)509758444 (DE-600)2228434-5 1555-6611 nnns volume:22 year:2012 number:8 day:09 month:07 pages:1335-1339 https://dx.doi.org/10.1134/S1054660X12080130 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_24 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_110 GBV_ILN_150 GBV_ILN_161 GBV_ILN_213 GBV_ILN_230 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2190 AR 22 2012 8 09 07 1335-1339 |
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10.1134/S1054660X12080130 doi (DE-627)SPR020141335 (SPR)S1054660X12080130-e DE-627 ger DE-627 rakwb eng Liu, M. verfasserin aut Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. Fiber Laser (dpeaa)DE-He213 Laser Physics (dpeaa)DE-He213 Slow Motion (dpeaa)DE-He213 Pulse Pump (dpeaa)DE-He213 Quiet Period (dpeaa)DE-He213 Zhang, H. T. aut Yan, P. aut Gong, M. L. aut Zheng, C. aut Meng, K. aut Enthalten in Laser physics Bristol [u.a.] : IOP Publ., 2006 22(2012), 8 vom: 09. Juli, Seite 1335-1339 (DE-627)509758444 (DE-600)2228434-5 1555-6611 nnns volume:22 year:2012 number:8 day:09 month:07 pages:1335-1339 https://dx.doi.org/10.1134/S1054660X12080130 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_24 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_110 GBV_ILN_150 GBV_ILN_161 GBV_ILN_213 GBV_ILN_230 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2190 AR 22 2012 8 09 07 1335-1339 |
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10.1134/S1054660X12080130 doi (DE-627)SPR020141335 (SPR)S1054660X12080130-e DE-627 ger DE-627 rakwb eng Liu, M. verfasserin aut Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. Fiber Laser (dpeaa)DE-He213 Laser Physics (dpeaa)DE-He213 Slow Motion (dpeaa)DE-He213 Pulse Pump (dpeaa)DE-He213 Quiet Period (dpeaa)DE-He213 Zhang, H. T. aut Yan, P. aut Gong, M. L. aut Zheng, C. aut Meng, K. aut Enthalten in Laser physics Bristol [u.a.] : IOP Publ., 2006 22(2012), 8 vom: 09. Juli, Seite 1335-1339 (DE-627)509758444 (DE-600)2228434-5 1555-6611 nnns volume:22 year:2012 number:8 day:09 month:07 pages:1335-1339 https://dx.doi.org/10.1134/S1054660X12080130 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_24 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_110 GBV_ILN_150 GBV_ILN_161 GBV_ILN_213 GBV_ILN_230 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2190 AR 22 2012 8 09 07 1335-1339 |
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10.1134/S1054660X12080130 doi (DE-627)SPR020141335 (SPR)S1054660X12080130-e DE-627 ger DE-627 rakwb eng Liu, M. verfasserin aut Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. Fiber Laser (dpeaa)DE-He213 Laser Physics (dpeaa)DE-He213 Slow Motion (dpeaa)DE-He213 Pulse Pump (dpeaa)DE-He213 Quiet Period (dpeaa)DE-He213 Zhang, H. T. aut Yan, P. aut Gong, M. L. aut Zheng, C. aut Meng, K. aut Enthalten in Laser physics Bristol [u.a.] : IOP Publ., 2006 22(2012), 8 vom: 09. Juli, Seite 1335-1339 (DE-627)509758444 (DE-600)2228434-5 1555-6611 nnns volume:22 year:2012 number:8 day:09 month:07 pages:1335-1339 https://dx.doi.org/10.1134/S1054660X12080130 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_24 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_110 GBV_ILN_150 GBV_ILN_161 GBV_ILN_213 GBV_ILN_230 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2190 AR 22 2012 8 09 07 1335-1339 |
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Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations Fiber Laser (dpeaa)DE-He213 Laser Physics (dpeaa)DE-He213 Slow Motion (dpeaa)DE-He213 Pulse Pump (dpeaa)DE-He213 Quiet Period (dpeaa)DE-He213 |
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Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations |
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Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations |
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Liu, M. |
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Liu, M. Zhang, H. T. Yan, P. Gong, M. L. Zheng, C. Meng, K. |
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Elektronische Aufsätze |
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Liu, M. |
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10.1134/S1054660X12080130 |
title_sort |
dynamics of yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations |
title_auth |
Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations |
abstract |
Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. © Pleiades Publishing, Ltd. 2012 |
abstractGer |
Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. © Pleiades Publishing, Ltd. 2012 |
abstract_unstemmed |
Abstract A special slow motion dynamic equations are presented especially adapt to the fiber laser analyze in which a long working cycle simulation and acute state changing are both needed. It can greatly save the calculation time while keep the output result relatively accurate. Then the dynamics of nanosecond high energy low repetition rate pulsed fiber amplifier is analyzed which indicate that most energy is wasted by means of self emission between pulses and the amplified self emission (ASE) is no longer the main cause of energy depletion with proper pulsed pump. Hence, unless a relatively large input seed source is used, the light conversion efficiency of a low repetition rate pulsed laser is usually much lower than the quantum efficiency even with a pulsed pump. © Pleiades Publishing, Ltd. 2012 |
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Dynamics of Yb-doped double clad pulsed fiber amplifier based on slow motion dynamic rate equations |
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