944 resultados para Q-Oscillator Algebra
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采用一种新型的被动调Q饱和吸收体,低温生长GaAs薄膜,实现了半导体抽运Nd:YVO4激光器的调Q运转.研究了激光器的调Q特性,调Q抽运阈值为2W.在抽运功率9.2 W时,获得的最短脉冲半峰全宽为15 ns,最大单脉冲能量为4.84 μJ,最高峰值功率为330 W,最大平均输出功率为1.16 W;脉冲重复频率在220 kHz到360 kHz之间.
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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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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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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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We reported a passive Q-switched diode laser pumped Yb:YAG microchip laser with an ion-implanted semi-insulating GaAs wafer. The wafer was implanted with 400-keV As^(+) in the concentration of 10^(16) ions/cm^(2). To decrease the non-saturable loss, we annealed the ion-implanted GaAs at 500 oC for 5 minutes and coated both sides of the ion-implanted GaAs with antireflection (AR) and highreflection (HR) films, respectively. Using GaAs wafer as an absorber and an output coupler, we obtained 52-ns pulse duration of single pulse.
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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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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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A passive Q-switched flash-lamp-pumped Nd:YAG laser with the ion-implanted semi-insulating GaAs water is reported.The wafer is implanted with 400keV As~+ ions in the concentration of 10~(16)cm~(-2). Using GaAs wafer as an absorber and an output coupler.62ns pulse duration of single pulse is obtained.
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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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This article proposes a new wake oscillator model for vortex induced vibrations of an elastically supported rigid circular cylinder in a uniform current. The near wake dynamics related with the fluctuating nature of vortex shedding is modeled based on the classical van der Pol equation, combined with the equation for the oscillatory motion of the body. An appropriate approach is developed to estimate the empirical parameters in the wake oscillator model. The present predicted results are compared to the experimental data and previous wake oscillator Model results. Good agreement with experimental results is found.
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Based on improving the wake-oscillator model, an analytical model for vortex-induced vibration (VIV) of flexible riser under non-uniform current is presented, in which the variation of added mass at lock-in and the nonlinear relationship between amplitude of response and reduced velocity are considered. By means of empirical formula combining iteration computation, the improved analytical model can be conveniently programmed into computer code with simpler and faster computation process than CFD so as to be suitable to application of practical engineering. This model is validated by comparing with experimental result and numerical simulation. Our results show that the improved model can predict VIV response and lock-in region more accurately. At last, illustrative examples are given in which the amplitude of response of flexible riser experiencing VIV under action of non-uniform current is calculated and effects of riser tension and flow distribution along span of riser are explored. It is demonstrated that with the variation of tension and flow distribution, lock-in region of mode behaves in different way, and thus the final response is a synthesis of response of locked modes.
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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.