227 resultados para Passively Q-switched


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采用低温生长GaAs晶体作为被动饱和吸收体兼输出镜,实现了Nd∶Gd0.42Y0.58VO4混晶激光器的调Q锁模运转。研究了Nd∶Gd0.42Y0.58VO4激光器的基频运转特性。在输出镜透射率T=10%、腔长L=40 mm的情况下,当抽运功率为8.6 W时,获得激光输出功率3.78 W,光光转换效率为43.9%。并测量了Nd∶Gd0.42Y0.58VO4混晶被动调Q激光器的输出特性。实验结果表明激光器调Q运转阈值为2 W,当抽运功率为3.7 W时,激光器出现调Q锁模行为;当抽运功率为8.6 W时,激光器调Q锁模深度达70%以上,对应的脉冲包络重复频率为670 kHz,半峰全宽为180 ns,平均输出功率为1.35 W,光光转换效率为15.7%。

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We report a diode end-pumped continuous wave (CW) passively mode-locked Nd:YVO4 laser with a homemade semiconductor saturable absorber mirror (SESAM). The maximum average output power is 5.3 W at the incident pump power of 17 W, which corresponds to an optical-optical conversion efficiency of 31.2% and slope efficiency of 34.7%. The corresponding optical spectrum has a 0.2-nm full width at half maximum (FWHM), and the pulse repetition rate is 83 MHz.

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锁模光纤激光器具有体积小、性能稳定及模式好等优点,日益受到关注。利用一种新型的透过式半导体可饱和吸收镜,实现双包层掺Yb^3+光纤激光器调Q锁模脉冲激光输出。得到的脉冲调Q包络半高宽约500ns,重复频率110kHz,平均输出功率45mW,锁模脉冲重复频率26.7MHz。锁模光路比反射式吸收镜更简单,易于调节,为进一步引入色散补偿元件进行飞秒脉冲的实验研究奠定了基础。

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利用金属有机气相淀积方法生长了一种新型吸收体:高反射率半导体可饱和吸收镜.用这种吸收体兼作端镜,实现了1.044μm半导体端面泵浦Yb∶YAB激光器被动锁模,脉冲宽度为3.05ps,重复率为375MHz,输出功率为45mW.

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制作了一种新型的半导体可饱和吸收镜--表面态型半导体可饱和吸收镜.用表面态型半导体可饱和吸收镜作为被动锁模吸收体实现了半导体端面泵浦Yb∶YAG激光器被动调Q锁模.在泵浦功率仅有1.4 W的情况下,获得了调Q锁模脉冲序列,锁模平均输出功率1 mW,锁模脉冲重复频率200 MHz.

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用离子注入的半绝缘GaAs晶片作为吸收体和输出镜,在双包层掺镱光纤激光器上实现了调Q锁模.离子注入的能量为400keV的As+离子,注入剂量为1016/cm2,然后在600℃下退火20min.当抽运功率为5W时,脉冲平均输出功率为200mW,调Q包络重复频率为50kHz,半高宽为4μs,锁模脉冲重复频率为15MHz。

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A novel InGaAs(LT-In0.25 Ga0.75 As) absorber grown by metal organic chemical vapor deposition at low temperature is presented.Using it as well as an output coupler,passive mode locking,which produces pulses as short as several hundred picoseconds for diode-end-pumped Nd∶YAG laser at 1.06μm,is realized.The pulse frequency is 150MHz.

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介绍了国际上流行的长波长半导体可饱和吸收镜的研制方法及其在固体激光器被动锁模和被动调Q中所起的作用,并分别就Cr4+:YAG,Cr:Forsterite等激光器进行了阐述.

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较全面介绍了几种掺钕激光晶体的光学性质。就掺钕激光晶体主要的三个波长探讨了用一种新型的吸收体(半导体可饱和吸收镜)进行被动调Q和锁模。

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于2010-11-23批量导入

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We present a novel system design that can generate the optimized wavelength-tunable optical pulse streams from an uncooled gain-switched Fabry-Perot semiconductor laser using an optical amplifier as external light source. The timing jitter of gain-switched laser has been reduced from about 3 ps to 600 fs and the pulse width has been optimized by using our system. The stability of the system was also experimentally investigated. Our results show that an uncooled gain-switched FP laser system can feasibly produce the stable optical pulse trains with pulse width of 18 ps at the repetition frequency of 5 GHz during 7 h continuous working. We respectively proved the system feasibility under 1 GHz, 2.5 GHz and 5 GHz operation. (c) 2008 Elsevier B.V. All rights reserved.

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We design a low-timing-jitter, repetition-rate-tunable, stretched-pulse passively mode-locked fiber laser by using a nonlinear amplifying loop mirror (NALM), a semiconductor saturable absorber mirror (SESAM), and a tunable optical delay line in the laser configuration. Low-timing-jitter optical pulses are stably produced when a SESAM and a 0.16 m dispersion compensation fiber are employed in the laser cavity. By inserting a tunable optical delay line between NALM and SESAM, the variable repetition-rate operation of a self-starting, passively mode-locked fiber laser is successfully demonstrated over a range from 49.65 to 50.47 MHz. The experimental results show that the newly designed fiber laser can maintain the mode locking at the pumping power of 160 mW to stably generate periodic optical pulses with width less than 170 fs and timing jitter lower than 75 fs in the 1.55 mu m wavelength region, when the fundamental repetition rate of the laser is continuously tuned between 49.65 and 50.47 MHz. Moreover, this fiber laser has a feature of turn-key operation with high repeatability of its fundamental repetition rate in practice.

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The total cross-section for the dd → 4HeK+K− reaction has been measured at a beam momentum of 3.7GeV/c, corresponding to an excess energy of 39MeV, which is the maximum possible atthe Cooler Synchrotron COSY-Jülich. A deuterium cluster-jet target and the ANKE forward magnetic spectrometer, placed inside the storage ring, have been employed in this investigation. We find a total cross-section of σtot < 14 pb, which brings into question the viability of investigating the dd → 4He a0(980)reaction as a means of studying isospin violation.