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SG-Ⅲ原型装置数十nm宽带数kJ输出能力评估 被引量:2
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作者 刘兰琴 张颖 +4 位作者 王文义 黄晚晴 谢旭东 耿远超 朱启华 《强激光与粒子束》 EI CAS CSCD 北大核心 2014年第9期182-185,共4页
利用现有窄带激光传输模拟软件sG99和宽带激光传输模拟软件cPAP,以及自编的一维光脉冲传输放大的逆算程序,评估了原型装置在主放基本结构不动的情况下激光脉冲由窄带改为宽带,实现数十nm宽带条件数kJ的输出能力。宽带下增益窄化效应... 利用现有窄带激光传输模拟软件sG99和宽带激光传输模拟软件cPAP,以及自编的一维光脉冲传输放大的逆算程序,评估了原型装置在主放基本结构不动的情况下激光脉冲由窄带改为宽带,实现数十nm宽带条件数kJ的输出能力。宽带下增益窄化效应显现,对光谱增益窄化补偿也进行了研究。结果表明,为了补偿增益窄化效应,在3J主放注入能量下通过对光谱整形可满足系统2000~3000J的输出,但损失约40%的注入能量。考虑到这一因素,预放级至少要有5J的输出能力。研究结果指导了数十nm宽带倍频激光驱动实验系统研制实施方案。 展开更多
关键词 宽带激光脉冲 传输放大 增益窄化补偿 输出能力
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宽带啁啾脉冲激光非线性传输过程中的时空微扰研究
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作者 王灿华 章礼富 +1 位作者 傅喜泉 文双春 《物理学报》 SCIE EI CAS CSCD 北大核心 2010年第9期6224-6230,共7页
基于非线性薛定谔方程推导出大啁啾脉冲的传输方程,利用微扰理论,分析了啁啾脉冲激光的时空不稳定性.理论上比较清楚的阐述了宽带脉冲激光在大啁啾情况下,其时空噪声的相互影响与相互作用情况及脉冲啁啾对噪声微扰调制的影响,发现在相同... 基于非线性薛定谔方程推导出大啁啾脉冲的传输方程,利用微扰理论,分析了啁啾脉冲激光的时空不稳定性.理论上比较清楚的阐述了宽带脉冲激光在大啁啾情况下,其时空噪声的相互影响与相互作用情况及脉冲啁啾对噪声微扰调制的影响,发现在相同γI0(非线性系数与峰值强度乘积)的情况下脉冲啁啾对噪声调制的增长没有直接影响.最后我们在实验上利用非线性介质对啁啾脉冲的空间小尺度自聚焦过程进行了部分验证,同时也在数值上对宽带啁啾脉冲的时间噪声调制的增长进行了模拟分析,发现实验结果和模拟分析结论都与理论分析基本一致. 展开更多
关键词 时空不稳定性 宽带脉冲激光 啁啾
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Ultra-Wideband Electromagnetic Radiation from GaAs Photoconductive Switches 被引量:2
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作者 施卫 贾婉丽 纪卫莉 《Journal of Semiconductors》 EI CAS CSCD 北大核心 2005年第1期11-15,共5页
The experiment results of ultrawide band electromagnetic radiation with DC biased GaAs photoconductive semiconductor switch combining double ridge horn antenna triggered by high repeat frequency femto-second laser pul... The experiment results of ultrawide band electromagnetic radiation with DC biased GaAs photoconductive semiconductor switch combining double ridge horn antenna triggered by high repeat frequency femto-second laser pulse are reported.The GaAs switches are insulated by solid multi-layer transparent dielectrics and the distance of two electrodes is 3mm.The electrode material of the switch is ohmic contact through alloy technics with definite proportion of Au/Ge/Ni.This switch and double ridge horn antenna are integrated and the receive antenna is connected with the test instrument.From receiving antenna,ultra fast electrical pulse of 200ps rise time and 500ps pulse width is obtained,the repetition rate of the pulse is about 82MHz and the frequency spectrum is in the range of 4.7MHz~14GHz.The radiation characteristic of the ultrafast electrical pulse is analyzed. 展开更多
关键词 GaAs photoconductive switch ultra-wideband microwave femto-second laser pulse
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Broadband isolated attosecond pulse generation in a two-color laser field combined with an orthogonally polarized laser pulse 被引量:2
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作者 DU HongChuan WANG XiaoShan HU BiTao 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2012年第1期1-6,共6页
We present a method to generate broadband isolated attosecond pulses. Using a two-color laser field, which is synthesized by a mid-infrared (12.5 fs, 2000 nm) and a weaker (12 fs, 800 nm) pulse in the x direction,... We present a method to generate broadband isolated attosecond pulses. Using a two-color laser field, which is synthesized by a mid-infrared (12.5 fs, 2000 nm) and a weaker (12 fs, 800 nm) pulse in the x direction, a modulated supercontinuum from 290 to 430 eV is obtainable. By properly adding a second-harmonic control field of the driving pulse in the y direction, the short quantum path is well selected and a smooth supercontinuum from 290 to 440 eV is generated. The bandwidth of the supercontinuum can be controlled by adjusting the electric field of the control pulse in the x direction. When the electric field increases to 0.051 a.u., a smooth supercontinuum from 295 to 520 eV is obtained. Using this method we expect that isolated 63-as attosecond pulses with tunable central wavelengths are straightforwardly obtained.We present a method to generate broadband isolated attosecond pulses. Using a two-color laser field, which is synthesized by a mid-infrared (12.5 fs, 2000 nm) and a weaker (12 fs, 800 nm) pulse in the x direction, a modulated supercontinuum from 290 to 430 eV is obtainable. By properly adding a second-harmonic control field of the driving pulse in the y direction, the short quantum path is well selected and a smooth supercontinuum from 290 to 440 eV is generated. The bandwidth of the supercontinuum can be controlled by adjusting the electric field of the control pulse in the x direction. When the electric field increases to 0.051 a.u., a smooth supercontinuum from 295 to 520 eV is obtained. Using this method we expect that isolated 63-as attosecond pulses with tunable central wavelengths are straightforwardly obtained. 展开更多
关键词 HHG SUPERCONTINUUM attosecond pulses
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