共查询到20条相似文献,搜索用时 15 毫秒
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Pulses of 20 ps duration from a 1536-nm erbium-doped fiber laser mode-locked at 10 MHz were soliton-compressed in a 1-km fiber to 1.5 ps. The pulses were then amplified in an erbium-doped fiber amplifier and compressed in a second fiber to less than 300 fs. Pulses give rise to stimulated Raman scattering in fibers; the direct output from the erbium fiber laser-amplifier has sufficient peak power to pump fiber Raman lasers. The sources can be made very compact and, with laser diode pumping, an all-fiber design can be realized. Such sources will find use in high-speed optical and electrooptical sampling instrumentation. Peak powers are high enough to study the nonlinear fiber effects that usually require a high-power Nd:YAG or color center laser 相似文献
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Rational harmonic mode locking takes place in an actively mode-locked fiber laser when the modulation frequency fm=(n+1/p)fc, where n and p are both integers and fc is the inverse of the cavity round-trip time, the 22nd order of rational harmonic mode locking has been observed when fm ≈1 GHz. An optical pulse train with a repetition rate of 40 GHz has been obtained using a modulation frequency fm=10 GHz. The theory of rational harmonic mode locking has also been developed. The stability of the mode-locked pulses is improved considerably when a semiconductor optical amplifier is incorporated into the fiber laser cavity. The supermode noise in the RF spectrum of a mode-locked laser is removed for a certain range of current in the semiconductor optical amplifier 相似文献
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Zhuyuan Wang Yiping Cui Binfeng Yun Changgui Lu 《Photonics Technology Letters, IEEE》2005,17(10):2044-2046
Simultaneous continuous-wave multiwavelength operation of a Raman fiber laser is demonstrated with sampled Bragg grating (SBG) at room temperature. The characteristics of multiwavelength fiber ring laser can be easily controlled by adjusting the parameters of the SBG, including the sampling period and the sampling length. In the proposed fiber laser, stable four oscillating wavelengths with 100- and 50-GHz spacing has been achieved, respectively, as well as five oscillating ones with a wavelength spacing of only 25 GHz by varying the sampling period of the SBG. 相似文献
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Shiquan Yang E.A. Ponomarev Xiaoyi Bao 《Photonics Technology Letters, IEEE》2005,17(2):300-302
We demonstrated a simple method to realize repetition-rate-doubling in a frequency modulation (FM) mode-locking fiber laser. The mode-locking of the laser is based on converting FM modulation to amplitude modulation by using a phase-modulated optical fiber loop mirror, which is formed by a phase modulator and an additional coupler only. With 40-GHz modulation, we obtained 80-GHz 1.74-ps transform-limited pulse train in the experiments. 相似文献
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Stoltz B. Osterberg U. Gomes A. Sibbett W. Taylor J. 《Lightwave Technology, Journal of》1986,4(1):55-57
Stimulated Raman scattering ofQ -switched and mode-locked Nd:YAG laser pulses at 1.06 μm in a 120-m-long single-mode fiber has been investigated experimentally. A Photochron IIA Synchrosan streak camera with picosecond resolution was used to give time resolved detection of the first four order Stokes-Raman pulses at 1.12, 1.18, 1.24, and 1.31 μm. It has been shown that in traversing the fiber the fundamental and the first two order Stokes were substantially shortened and that the Stokes pulses were asymmetrical with sharper leading edges. 相似文献
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Smoothly wavelength-tunable picosecond pulse generation using a harmonically mode-locked fiber ring laser 总被引:1,自引:0,他引:1
A simple design of a stable, smoothly wavelength-tunable picosecond pulse generator has been demonstrated using a dispersion-tuned, harmonically mode-locked fiber ring laser with a directly modulated semiconductor optical amplifier (SOA). The SOA functions as both a polarization-insensitive mode locker and a supermode noise suppressor. Near-linearly chirped pulses are generated and compressed to less than 4 ps when the intracavity dispersion is anomalous while 11-ps, near-transform-limited pulses are generated without compression when the dispersion is normal. Smooth wavelength tuning is achieved over more than 11 nm by only tuning the modulation frequency and pulse characteristics are stable over the entire tuning span. A simple numerical model successively simulates the operation principle of the system. The tuning range is determined by both the gain profile and the total intracavity dispersion. The dispersion and the SOA ensure the long-term stability of the system. 相似文献
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Single-pass Raman generation pumped by a mode-locked Nd:YAG laser is investigated for long-span and low-loss fibres. The peak wavelength of the first Stokes jumps dramatically from 1.114 ?m to 1.12 ?m at 1.65 W average input power. The first Stokes increases rapidly between the inputs of 1.65 W and 2.1 W. These characteristics of single-pass stimulated Raman scattering are discussed in terms of group velocity matching. 相似文献
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Distributed feedback fiber Raman laser 总被引:1,自引:0,他引:1
We analyze the properties of a distributed feedback fiber laser based on Raman amplification. Such a laser is quite practical and has a number of novel properties. We model numerically the laser dynamics, analyze in detail the role of the nonlinear refractive index of the fiber and argue on the optimal design parameters 相似文献
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A fiber Raman ring laser was synchronously pumped by a cavity-dumped argon laser. The Raman laser was tuned with either a piezoelectric intracavity interferometer or by varying the pump pulse rate. 相似文献
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Ahmad H. A. Rosol Afiq A. A. Jafry Norrima Mokhtar Moh Yasin Sulaiman Wadi Harun 《光电子快报》2021,17(8):449-453
Passively Q-switched thulium doped fiber laser (TDFL) has been successfully demonstrated using gold nanoparticles (GNPs), which were embedded into polyvinyl alcohol as saturable absorber (SA). The stable self-starting Q-switched laser was generated to operate at 1 891 nm when a tiny piece of the prepared film was slot in between two fiber ferrules and incorporated into the laser cavity. The repetition rate can be adjusted from 48.54 kHz to 49.64 kHz while the pulse width decreased from 3.52 μs to 2.38 μs with the increase of 1 550 nm pump power from 840 mW to 930 mW. The corresponding pump power output power linearly increased from 3.62 mW to 6.3 mW with a slope efficiency of 2.53%. The maximum peak power and pulse energy were recorded at about 39 mW and 0.12 µJ, respectively at pump power of 930 mW. The Q-switching operation was caused by the surface plasmon resonance absorption of GNPs. 相似文献
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报道了一种全光纤超宽带光谱的类噪声脉冲锁模光纤激光器。为了加宽锁模光谱,利用腔内色散管理和非线性技术,使在58m腔内具有小的反常色散,平均色散系数为0.12 ps/nm/km。实验获得了超过1300nm--1750nm超宽带光谱锁模类噪声脉冲,光谱20-dB带宽达到362nm,3-dB带宽达到102nm。类噪声脉冲的光谱宽度远超过掺铒光纤的增益带宽。 相似文献
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Abraham D. Nagar R. Ruberto M.N. Eisenstein G. Koren U. Zyskind J.L. DiGiovanni D.J. 《Photonics Technology Letters, IEEE》1993,5(4):377-379
The authors demonstrate optical frequency tuning by direct electrical means as well as FM and AM mode-locking in an erbium-doped fiber laser with an intracavity distributed Bragg reflector active filter/modulator. They obtained a 6 nm discrete tuning range and pulses of 38 and 78 ps duration in AM and FM mode-locking, respectively 相似文献
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High-power supercontinuum generation in a nested linear cavity involving a CW Raman fiber laser 总被引:1,自引:0,他引:1
M. Feng Y.G. Li J. Li J.F. Li L. Ding K.C. Lu 《Photonics Technology Letters, IEEE》2005,17(6):1172-1174
We construct a novel nested linear cavity configuration to generate supercontinuum (SC) under continuous-wave pump. With this structure, stimulated Raman scattering and four-wave mixing can affect the whole region of the SC spectrum while the pump line is removed outside of the continuum, and a symmetrical spectrum can be obtained. The properties of the structure are demonstrated by using 3.5-km single-mode fiber, and an SC centered at 1315 nm with the bandwith of 102 nm and the output power of 1.3 W is achieved. By tuning the feedback fiber Bragg grating, we can easily adjust the spectral shape of SC to fit different requirement. 相似文献
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Supercontinuum(SC) generation in a dispersion-shifted fiber(DSF) pumped by a 10 GHz regeneratively mode-locked fiber laser(RMLFL) is presented. Optimization of pump wavelength leads to a 20 dB bandwidth of 58.73 nm,which covers the whole C band and part of L band. Using an angle-tuning thin film filter, multi-wavelength and pico-second pulse trains of low chirp could be chosen from the SC spectrum. Amplified spontaneous emission(ASE) induced degeneration of the achieved pulse trains is observed and discussed. 相似文献
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半导体激光器生成双波长超窄脉冲的实验研究 总被引:1,自引:0,他引:1
描述了一种用腔外注入方式调制增益的法布里珀罗半导体激光器产生双波长超窄脉冲的简单方法,腔外注入功能部分包含一个直流工作的法面里珀罗半导体激光器,一个3dB光耦合器和两个布喇格型光纤光栅。双波长的选择和间距通过调节光栅为实现,文中描述的系统实现了在10nm的调节范围内边模压制率优于17dB的理想结果。整个系统简单、成本低。 相似文献
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A c.w. GaAlAs laser is modelocked by gain modulation. 60 ps coherent pulses are obtained at a repetition frequency of 433 MHz. 相似文献
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Shiquan Yang E.A. Ponomarev Xiaoyi Bao 《Photonics Technology Letters, IEEE》2004,16(7):1631-1633
A 40-GHz frequency modulation oscillation fiber laser is demonstrated and the continuous-wave (CW) output is used for generating a high repetition rate short pulse train by external cavity chirp compensation. A 1.37-ps transform-limited pulse is obtained from its chirped, 488.1-GHz width CW output. 相似文献