首页> 外文期刊>PHYSICAL REVIEW A >High-order harmonic generation in Xe, Kr, and Ar driven by a 2.1-μm source: High-order harmonic spectroscopy under macroscopic effects
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High-order harmonic generation in Xe, Kr, and Ar driven by a 2.1-μm source: High-order harmonic spectroscopy under macroscopic effects

机译:由2.1μm光源驱动的Xe,Kr和Ar中的高次谐波产生:宏观效应下的高次谐波光谱

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摘要

We experimentally and numerically study the atomic response and pulse propagation effects of high-ordernharmonics generated in Xe, Kr, and Ar driven by a 2.1-μm infrared femtosecond light source. The light source isnan optical parametric chirped-pulse amplifier, and a modified strong-field approximation and three-dimensionalnpulse propagation code are used for the numerical simulations. The extended cutoff in the long-wavelength-drivennhigh-order harmonic generation has revealed the spectral shaping of high-order harmonics due to the atomicnstructure (or photorecombination cross section) and the macroscopic effects, which are the main factors ofndetermining the conversion efficiency besides the driving wavelength. Using precise numerical simulations tondetermine the macroscopic electron wave packet, we are able to extract the photorecombination cross sectionsnfrom experimental high-order harmonic spectra in the presence of macroscopic effects. We have experimentallynobserved that the macroscopic effects shift the observed Cooper minimum of Kr from 80 eV to 60–70 eV andnwash out the Cooper minimum of Ar. Measured high-harmonic conversion efficiencies per harmonic near thencutoff are ∼10−9 for all three gases.
机译:我们通过实验和数值研究了由2.1μm红外飞秒光源驱动的Xe,Kr和Ar中产生的高次谐波的原子响应和脉冲传播效应。光源为南光参量chi脉冲放大器,采用改进的强场近似和三维脉冲传播码进行数值模拟。在长波驱动的高次谐波产生中,延长的截止频率揭示了由于原子结构(或光重组截面)和宏观效应引起的高次谐波的频谱整形,这是确定转换效率的主要因素。驱动波长。使用精确的数值模拟来确定宏观电子波包,我们能够在存在宏观效应的情况下从实验性高次谐波光谱中提取光重组截面n。我们从实验上观察不到宏观效应将观察到的Kr的Cooper最小值从80 eV转移到60-70 eV,并冲走了Ar的Cooper最小值。对于所有三种气体,在截止时附近每个谐波测得的高谐波转换效率约为10-9。

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  • 来源
    《PHYSICAL REVIEW A》 |2012年第4期|1-10|共10页
  • 作者单位

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USA;

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USA;

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USA;

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USA;

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USA;

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USAIKERBASQUE Basque Foundation for Science Spain;

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USA;

    Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics Massachusetts Institute of Technology(MIT) Cambridge Massachusetts 02139 USACenter for Free-Electron Laser Science DESY and Department of Physics Hamburg University Notkestraße 85 D-22607 HamburgGermany;

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  • 入库时间 2022-08-17 13:56:22

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