Divided-Pulse Nonlinear Amplification at 1.5 μm
Divided-pulse nonlinear amplification was developed in the anomalous dispersion regime by combining the concepts of divided-pulse nonlinear amplification and divided-pulse compression. We realized compressor-free ultrafast pulse amplifiers at 1.5 μm with the help of simultaneous pulse amp...
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doaj-a582fc1d1c424e7b88084a083ce27df82021-03-29T17:35:57ZengIEEEIEEE Photonics Journal1943-06552016-01-01851810.1109/JPHOT.2016.26032337553574Divided-Pulse Nonlinear Amplification at 1.5 μmQiang Hao0Yunfeng Wang1Tingting Liu2Hong Hu3Heping Zeng4Shanghai Key Laboratory of Modern Optical Systems, Engineering Research Center of Optical Instruments and Systems, Ministry of Education, School of Optical Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai, ChinaShanghai Key Laboratory of Modern Optical Systems, Engineering Research Center of Optical Instruments and Systems, Ministry of Education, School of Optical Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai, ChinaShanghai Key Laboratory of Modern Optical Systems, Engineering Research Center of Optical Instruments and Systems, Ministry of Education, School of Optical Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai, ChinaDepartment of Respiratory Medicine, Chinese PLA General Hospital, Beijing, ChinaShanghai Key Laboratory of Modern Optical Systems, Engineering Research Center of Optical Instruments and Systems, Ministry of Education, School of Optical Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai, ChinaDivided-pulse nonlinear amplification was developed in the anomalous dispersion regime by combining the concepts of divided-pulse nonlinear amplification and divided-pulse compression. We realized compressor-free ultrafast pulse amplifiers at 1.5 μm with the help of simultaneous pulse amplification and compression in single-mode and few-mode fibers with anomalous dispersion. With optimized positive prechirping on the seed pulse, the interplay between the dispersive and nonlinear effects was controlled to get transform-limited soliton replicas. Experiments, as well as numerical simulations, demonstrated that ~0.75 nJ per replica was the optimized results in the 12/130 Er-Yb codoped fiber. By polarization-division multiplexing 32 replicas, transform-limited pulse with 126-fs duration, 20.3-nJ pulse energy, and 80-MHz repetition rate was generated from a few-mode Er-Yb codoped fiber. Furthermore, limitations on the coherent combining efficiency are discussed.https://ieeexplore.ieee.org/document/7553574/Fiber Laserserbium laserslaser amplifierspulse compression. |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Qiang Hao Yunfeng Wang Tingting Liu Hong Hu Heping Zeng |
spellingShingle |
Qiang Hao Yunfeng Wang Tingting Liu Hong Hu Heping Zeng Divided-Pulse Nonlinear Amplification at 1.5 μm IEEE Photonics Journal Fiber Lasers erbium lasers laser amplifiers pulse compression. |
author_facet |
Qiang Hao Yunfeng Wang Tingting Liu Hong Hu Heping Zeng |
author_sort |
Qiang Hao |
title |
Divided-Pulse Nonlinear Amplification at 1.5 μm |
title_short |
Divided-Pulse Nonlinear Amplification at 1.5 μm |
title_full |
Divided-Pulse Nonlinear Amplification at 1.5 μm |
title_fullStr |
Divided-Pulse Nonlinear Amplification at 1.5 μm |
title_full_unstemmed |
Divided-Pulse Nonlinear Amplification at 1.5 μm |
title_sort |
divided-pulse nonlinear amplification at 1.5 μm |
publisher |
IEEE |
series |
IEEE Photonics Journal |
issn |
1943-0655 |
publishDate |
2016-01-01 |
description |
Divided-pulse nonlinear amplification was developed in the anomalous dispersion regime by combining the concepts of divided-pulse nonlinear amplification and divided-pulse compression. We realized compressor-free ultrafast pulse amplifiers at 1.5 μm with the help of simultaneous pulse amplification and compression in single-mode and few-mode fibers with anomalous dispersion. With optimized positive prechirping on the seed pulse, the interplay between the dispersive and nonlinear effects was controlled to get transform-limited soliton replicas. Experiments, as well as numerical simulations, demonstrated that ~0.75 nJ per replica was the optimized results in the 12/130 Er-Yb codoped fiber. By polarization-division multiplexing 32 replicas, transform-limited pulse with 126-fs duration, 20.3-nJ pulse energy, and 80-MHz repetition rate was generated from a few-mode Er-Yb codoped fiber. Furthermore, limitations on the coherent combining efficiency are discussed. |
topic |
Fiber Lasers erbium lasers laser amplifiers pulse compression. |
url |
https://ieeexplore.ieee.org/document/7553574/ |
work_keys_str_mv |
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1724197645415612416 |