共查询到20条相似文献,搜索用时 62 毫秒
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增益开关半导体激光器产生的光脉冲宽度往往较宽,且具有一定大小的脉冲基座。为了提高增益开关半导体激光器的脉冲质量,提出了一种三级脉冲整形方案。首先,利用色散补偿光纤将增益开关半导体激光器输出的光脉冲宽度从39.381 ps压缩到26.681 ps,随后利用掺铒光纤放大器和色散位移光纤的高阶孤子效应进一步将光脉冲的宽度压缩到20.916 ps,最后利用半导体光放大器的自相位调制效应区分开脉冲基座与脉冲中心的光谱,并利用光滤波器滤除脉冲基座对应的光谱部分,从而消减脉冲基座,并将脉冲宽度压缩到18.497 ps。实验结果表明,该三级脉冲整形方案可以有效地压缩脉冲宽度以及减小脉冲基座,从而提高增益开关半导体激光器输出光脉冲的质量。 相似文献
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为了满足大功率半导体激光器脉冲应用的实际需求, 针对单脉冲内电流平顶下降问题和重复性情况下电流稳定性降低的问题, 设计了一种多参数宽范围可调的高精度高稳定脉冲驱动电源。该电源以大功率场效应晶体管为核心, 通过现场可编程门阵列产生的高精度时序波形来完成单脉冲内的上升沿调控和栅极控制电压补偿, 通过微控制器结合电流采样的闭环控制方案实现重频运行下的电流高稳定输出。结果表明, 在输出电流100 A、脉冲宽度400 μs、重复频率1 kHz的最大功率输出驱动二极管负载时, 驱动电流上升沿过冲幅度小于0.5%、单脉冲内电流衰减小于0.2%、重复率脉冲不稳定度小于0.1%;在同样输出条件下驱动半导体激光器, 其在单脉冲内光功率过冲小于2%, 重复光脉冲不稳定度小于0.2%。该研究有助于提高脉冲电源脉冲电流稳定性, 对现有脉冲电源结构的改进具有一定的参考意义。 相似文献
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本文概述半导体激光器皮秒(ps)光脉冲产生的方法,这些方法包括锁模、增益开关、电反馈、光电反馈和Q开关等,并报道了各种方法产生ps光脉冲的现有水平及未来展望。 相似文献
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To obtain high power, well shaped picosecond pulses from gain-switched semiconductor lasers, the use of dynamic gain saturation characteristics of semiconductor laser amplifiers was investigated theoretically and experimentally. A configuration of a reflected-wave amplifier (RWA) with single-side external coupling is introduced for pulse shaping, which is found to be suitable for enhancing dynamic gain saturation. By a combination of a distributed feedback laser oscillator at 1.3 μm in wavelength and a reflected-wave amplifier of 400 μm cavity length with asymmetric facet reflectivities of 0.01% and 30%, single-mode optical pulses with almost no tailing, full width at half maximum of 15 ps, and peak power exceeding 50 mW were obtained without pulse broadening, despite the considerable tail structure of the incident pulse 相似文献
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Optical processing based on spectral line-by-line pulse shaping on a phase-modulated CW laser 总被引:1,自引:0,他引:1
We demonstrate optical processing based on spectral line-by-line pulse shaping of a frequency comb generated by phase modulating a CW laser and show various applications including CW-to-pulse conversion, width/wavelength tunable return-to-zero pulse generation, pulse-to-CW conversion, wavelength conversion, and microwave photonics. The correlations between optical spectra, time-domain waveforms, and RF spectra are quantitatively studied. 相似文献
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PAPR reduction based on improved Nyquist pulse shaping technology in OFDM-RoF systems 总被引:1,自引:0,他引:1
High peak-to-average power ratio (PAPR) is the main disadvantage in orthogonal frequency-division multiplexing (OFDM) communication systems, which also exists in OFDM-radio over fiber (RoF) systems. In this paper, we firstly analyze the impact of high PAPR on a 40 GHz OFDM-RoF system, and then describe the theory of Nyquist pulse shaping technology for reducing PAPR. To suppress PAPR further, an improved Nyquist pulse shaping technology is proposed, in which the distribution of original-data amplitude is changed by properly selecting the time-limited waveforms of the different subcarriers. We firstly apply the improved Nyquist pulse shaping technology to an OFDM-RoF system. The simulation results show that PAPR is effectively reduced by more than 2 dB with the bit error rate (BER) declining by about 0.125%. 相似文献
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Optical pulse shaping by cross-phase modulation in a harmonic mode-locked semiconductor fiber ring laser under large cavity detuning 总被引:1,自引:0,他引:1
Chung Ghiu Lee Yun Jong Kim Chang-Soo Park 《Lightwave Technology, Journal of》2006,24(3):1237-1246
The authors experimentally investigate the phenomena of the pulse-shape distortion due to the drift of cavity length or modulation frequency in a harmonically mode-locked semiconductor fiber ring laser (SFRL). Also, it is experimentally demonstrated that the optical pulse shaping by cross-phase modulation (XPM) can be applied to enhance the robustness of a harmonic mode-locked semiconductor ring laser to the environmental factors, e.g., the modulation-frequency drift and/or the cavity-length drift. The mechanism of pulse-shape distortion due to the modulation-frequency drift or cavity-length drift is explained and experimentally verified. As the locking condition of the SFRL goes to the rational harmonic mode-locking (RHML) regime, the pulse-shape distortion becomes dominant. To validate the explanation, a simple equation for estimating and comparing the amount of cavity-length detuning in terms of frequency is proposed for comparison, which is called the equivalent frequency detuning (EFD). The distortion mostly appeared in the trailing edge of the pulse. By selectively filtering the XPM-induced red-chirped wavelength components in the rising edge of the pulse, the mode-locked pulse train with large pulse-shape distortion can be reshaped to regenerate a mode-locked pulse train with less pulse-shape distortion than the pulse train without the proposed scheme. This method can be used to reduce the pulse-shape distortion effectively, maintaining the pulse repetition rate under the large modulation-frequency detuning, or equivalently, large cavity-length detuning. The proposed scheme is able to generate the pulse-trains robust to the modulation-frequency drift and/or cavity-length drift of the mode-locked SFRL. 相似文献
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