High-Pulse-Energy All-Normal-Dispersion Yb-Doped Fiber Laser Based on Nonlinear Polarization Evolution*Supported by the National Key Scientific Instruments Development Program of China Under Grant No 2012YQ120047

High-Pulse-Energy All-Normal-Dispersion Yb-Doped Fiber Laser Based on Nonlinear Polarization Evolution*Supported by the National Key Scientific Instruments Development Program of China Under Grant No 2012YQ120047 PDF Author:
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Languages : en
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Abstract : We report an all-normal-dispersion ytterbium fiber laser mode locked by nonlinear polarization evolution. With a 347-m-long all-fiber ring cavity, a pulse energy of 263 nJ at a repetition rate of 613kHz is achieved, which is the highest per-pulse energy directly obtained from an all-fiber mode-locked laser doped by ytterbium ions. The compact and operation-robust laser yields a well-shaped spectrum centered at 1032 nm with a bandwidth (FWHM) of 4 nm, and the slope efficiency is as high as 27.5%. The proposed low-repetition-rate high-pulse-energy mode-locked fiber laser will be a promising seed for all-fiber chirped pulsed amplification systems.

High-Pulse-Energy All-Normal-Dispersion Yb-Doped Fiber Laser Based on Nonlinear Polarization Evolution*Supported by the National Key Scientific Instruments Development Program of China Under Grant No 2012YQ120047

High-Pulse-Energy All-Normal-Dispersion Yb-Doped Fiber Laser Based on Nonlinear Polarization Evolution*Supported by the National Key Scientific Instruments Development Program of China Under Grant No 2012YQ120047 PDF Author:
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Languages : en
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Abstract : We report an all-normal-dispersion ytterbium fiber laser mode locked by nonlinear polarization evolution. With a 347-m-long all-fiber ring cavity, a pulse energy of 263 nJ at a repetition rate of 613kHz is achieved, which is the highest per-pulse energy directly obtained from an all-fiber mode-locked laser doped by ytterbium ions. The compact and operation-robust laser yields a well-shaped spectrum centered at 1032 nm with a bandwidth (FWHM) of 4 nm, and the slope efficiency is as high as 27.5%. The proposed low-repetition-rate high-pulse-energy mode-locked fiber laser will be a promising seed for all-fiber chirped pulsed amplification systems.

Fabrication of 16 W All-normal-dispersion Mode-locked Yb-doped Rod-type Fiber Laser with Large-mode Area*Project Supported by the National Key Technology R&D Program of the Ministry of Science and Technology, China (Grant No. 2012BAC23B03), the National Basic Research Program of China (Grant No. 2013CB922401), and the National Natural Science Foundation of China (Grant No. 11474002).

Fabrication of 16 W All-normal-dispersion Mode-locked Yb-doped Rod-type Fiber Laser with Large-mode Area*Project Supported by the National Key Technology R&D Program of the Ministry of Science and Technology, China (Grant No. 2012BAC23B03), the National Basic Research Program of China (Grant No. 2013CB922401), and the National Natural Science Foundation of China (Grant No. 11474002). PDF Author:
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Languages : en
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Yb-doped Passively Mode-locked Fiber Laser with Bi2Te3-deposited*Project Supported by the National Natural Science Foundation of China (Grant No. 61378024) and the Natural Science Fund of Guangdong Province, China (Grant No. S2013010012235).

Yb-doped Passively Mode-locked Fiber Laser with Bi2Te3-deposited*Project Supported by the National Natural Science Foundation of China (Grant No. 61378024) and the Natural Science Fund of Guangdong Province, China (Grant No. S2013010012235). PDF Author:
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Languages : en
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Abstract: In this study we present an all-normal-dispersion Yb-doped fiber laser passively mode-locked with topological insulator (Bi2 Te3 ) saturable absorber. The saturable absorber device is fabricated by depositing Bi2 Te3 on a tapered fiber through using pulsed laser deposition (PLD) technology, which can give rise to less non-saturable losses than most of the solution processing methods. Owing to the long interaction length, Bi2 Te3 is not exposed to high optical power, which allows the saturable absorber device to work in a high power regime. The modulation depth of this kind of saturable absorber is measured to be 10%. By combining the saturable absorber device with Yb-doped fiber laser, a mode-locked pulse operating at a repetition rate of 19.8 MHz is achieved. The 3-dB spectral width and pulse duration are measured to be 1.245 nm and 317 ps, respectively.

High-Energy YB-Doped Femtosecond Fiber Lasers

High-Energy YB-Doped Femtosecond Fiber Lasers PDF Author: Hussein Kotb
Publisher:
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Category : Energy dissipation
Languages : en
Pages :

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The main objective of the thesis is to understand the parameters that contribute in limiting the pulse energy and spectral bandwidth of the mode-locked femtosecond fiber lasers. I have focused on studying the impact of the parameters of the saturable absorber and the bandwidth of the lumped spectral filter on the temporal and spectral profiles of the pulse. Therefore, I developed two models that can help us to optimize the pulse characteristics such as the pulse energy, spectral bandwidth and de-chirped pulse width. I also introduce two techniques that result in increasing the pulse peak power and spectral bandwidth. The nonlinear transmission coefficient of the saturable absorber is one of the main limitations to achieving high-energy pulses. Throughout my research, I have used two types of saturable absorbers. The first is a lumped semiconductor saturable absorber mirror (SESAM) and the second is based on the nonlinear polarization rotation (NPR) that is considered an artificial saturable absorber with distributed effect. The first model introduced in this thesis is an analytical model, which provides closed form relations for the pulse characteristics of all-normal dispersion fiber laser. It shows how the spectral bandwidth of the lumped filter inserted inside the cavity affects the pulse characteristics. Also, it illustrates the influence of the saturable absorber parameters on the pulse characteristics. I show that increasing the small signal saturable absorber loss and decreasing the saturation power leads to the increase in pulse energy and spectral bandwidth. Numerical simulation and experimental results are in agreement with the results of the analytical models. The second model, which is called the semi-vector model, is applicable to all-normal dispersion mode-locked fiber laser with high output coupling ratio. Nonlinear polarization rotation is employed for mode-locking. The model shows the relationship between the location of the overdriving point of the saturable absorber and the output pulse energy. The results of this model are in agreement with those of the full-vector model, but with a much reduced simulation time. In addition, the experimental results show the accuracy of the proposed model. In this thesis, I mitigate the peak power limitation, caused by the accumulated nonlinear phase shift, by replacing the short high-doped Yb3+ fiber with a long low-doped one. This results in an increase of the peak power by a factor that depends on the ratio between the gain coefficient of the high- and low-doped Yb3+ fiber. The length of the nonlinear section is kept unchanged by reducing the length of the single mode fiber after the long low-doped Yb3+ fiber. Numerical simulation and experimental results validate the idea. The location of narrow bandwidth lumped spectral filter, in an active Similariton laser, has proved to have a distinct effect on the pulse energy, spectral bandwidth and de-chirped pulse width and peak power. The proximity of the spectral filter to the input of the Yb3+-doped fiber leads to increasing the pulse spectral bandwidth and peak power of the de-chirped pulse as well as shortening the de-chirped pulse, but at the expense of reducing the pulse energy.

Pulsed Fiber Lasers

Pulsed Fiber Lasers PDF Author: Peter Adel
Publisher: Cuvillier Verlag
ISBN: 3865371469
Category :
Languages : en
Pages : 170

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Wideband All-Polarization-Maintaining Yb-Doped Mode-Locked Fiber Laser Using a Nonlinear Optical Loop Mirror

Wideband All-Polarization-Maintaining Yb-Doped Mode-Locked Fiber Laser Using a Nonlinear Optical Loop Mirror PDF Author:
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Languages : en
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Abstract : We report on a wide-band and stable mode-locked all-polarization-maintaining fiber laser configuration using a nonlinear optical loop mirror. The central wavelength of the laser is 1080.14 nm and the 3 dB bandwidth is 20.29 nm. The repetition rate of the pulse is 3.28 MHz and the pulse width is 848 ps. By tuning the pump power, which is centered at 980 nm, from 300 mW to 380 mW, we obtain a linearly changed output power from 6mW to 7.12 mW. The all-polarization-maintaining fiber configuration is fundamental to the stability of the output power.

All-Fiber, All-Normal-Dispersion,P-APM High Power Yb-doped Fiber Laser System

All-Fiber, All-Normal-Dispersion,P-APM High Power Yb-doped Fiber Laser System PDF Author:
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Category :
Languages : en
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High-Energy and Short-Pulse Generation from Passively Mode- Locked Ytterbium-Doped Double-Clad Fiber Lasers

High-Energy and Short-Pulse Generation from Passively Mode- Locked Ytterbium-Doped Double-Clad Fiber Lasers PDF Author: Yuzhai Pan
Publisher:
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Category : Science
Languages : en
Pages :

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Book Description
Mode-locked ytterbium-doped fiber lasers capable of producing nanosecond-, picosecond- or femtosecond-level pulses with high energy or power have many advantages for various applications such as material processing and laser surgery. Firstly, in this chapter, the principles and methods used in passively mode-locked fiber lasers are briefly described. Secondly, mathematical modeling of all normal dispersion ytterbium-doped fiber lasers for analyzing the pulse generation and propagation has been established and simulated with the generalized nonlinear Schrödinger equation. Thirdly, short pulses generated from passively mode-locked fiber lasers have been demonstrated with carbon nanotube- deposited D-shaped fiber as the saturable absorber. Different pulse width can be realized with different parameters of the laser cavity. Finally, the main amplification methods for short laser pulses have been discussed, and a broad prospect for applications of various technologies using short-pulse fiber lasers is further introduced.

Fiber Laser

Fiber Laser PDF Author: Mukul Paul
Publisher: BoD – Books on Demand
ISBN: 9535122576
Category : Technology & Engineering
Languages : en
Pages : 442

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Book Description
This book is a self-contained collection of scholarly papers targeting an audience of practicing researchers, academics, PhD students, and other scientists. This book describes the rapidly developing field of fiber laser technology filling the very important role of providing students, researchers, and technology managers with valuable, timely, and unbiased information on the subject. The objective of this book is to highlight recent progress and trends in fiber laser technology covering a wide range of topics, such as self-pulsing phenomena in high-power continuous wave (CW) Yb-doped fiber lasers, Q-switched fiber laser, mode-locked fiber laser using carbon nanotubes (CNT), properties of double-scale pulses in mode-locked fiber laser, Brillouin fiber laser, dual-wave length fiber laser (DWFL) for microwave (MHz) and terahertz (THz) radiation generation, tunable fiber laser based on twin core optical fiber, reflective semiconductor optical amplifier (RSOA)-based fiber laser, dissipative soliton phenomena in fiber lasers, noiselike pulses (NLPs) in Yb-doped fiber laser, ultra fast fiber laser, numerical simulation in Q-switched and mode-locked fiber laser, gain saturation in optical fiber laser amplifiers, heat generation and removal in fiber lasers, and different fiber laser based technologies for material processing. We hope that this book will be useful for students, researchers, and professionals, who work with fiber lasers. This book will also serve as an interesting and valuable reference that will impact, stimulate, and promote further advances in the area of fiber lasers

A Single-Frequency Linearly Polarized Fiber Laser Using a Newly Developed Heavily Tm3+-Doped Germanate Glass Fiber at 1.95 Μm*Supported by the National High-Technology Research and Development Program of China Under Grant Nos 2013AA031502 and 2014AA041902, the National Natural Science Foundation of China Under Grant Nos 11174085, 51132004, and 51302086, the Natural Science Foundation of Guangdong Province Under Grant Nos S2011030001349 and S20120011380, the China National Funds for Distinguished Young Scientists Under Grant No 61325024, the Science and Technology Project of Guangdong Province Under Grant No 2013B090500028, and the 'Cross and Cooperative' Science and Technology Innovation Team Project of Chinese Academy of Sciences Under Grant

A Single-Frequency Linearly Polarized Fiber Laser Using a Newly Developed Heavily Tm3+-Doped Germanate Glass Fiber at 1.95 Μm*Supported by the National High-Technology Research and Development Program of China Under Grant Nos 2013AA031502 and 2014AA041902, the National Natural Science Foundation of China Under Grant Nos 11174085, 51132004, and 51302086, the Natural Science Foundation of Guangdong Province Under Grant Nos S2011030001349 and S20120011380, the China National Funds for Distinguished Young Scientists Under Grant No 61325024, the Science and Technology Project of Guangdong Province Under Grant No 2013B090500028, and the 'Cross and Cooperative' Science and Technology Innovation Team Project of Chinese Academy of Sciences Under Grant PDF Author:
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Languages : en
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Abstract A compact linearly polarized, low-noise, narrow-linewidth, single-frequency fiber laser at 1950 nm is demonstrated. This compact fiber laser is based on a 21-mm-long homemade Tm3+-doped germanate glass fiber. Over 100-mW stable continuous-wave single transverse and longitudinal mode lasing at 1950 nm are achieved. The measured relative intensity noise is less than −135 dB/Hz at frequencies over 5 MHz. The signal-to-noise ratio of the laser is larger than 72 dB, and the laser linewidth is less than 6 kHz, while the obtained linear polarization extinction ratio is higher than 22 dB.