Controlling the contributions to high-order harmonic generation from different nuclei of N-2 with an orthogonally polarized two-color laser field

Controlling the contributions to high-order harmonic generation from different nuclei of N-2 with an orthogonally polarized two-color laser field
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用正交偏振双色激光场控制 N-2 不同核对高次谐波产生的贡献

DOI:
10.1088/1674-1056/25/9/093202
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发表时间:
2016-07
期刊:
影响因子:
1.7
通讯作者:
Liu Xue-Shen
Liu Xue-Shen
中科院分区:
物理与天体物理3区
文献类型:
--
作者:
Du Hui;Pan Xue-Fei;Liu Hai-Feng;Zhang Hong-Dan;Zhang Jun;Guo Jing;Liu Xue-Shen

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利用强场Lewenstein模型研究了N-2分子在正交偏振双色激光场中的高次谐波和阿秒脉冲的产生。结果表明,通过适当选择相对相位,可以实现对不同核对高次谐波产生贡献的控制。当相对相位取φ = 0.4 π时,一个核对高次谐波的贡献远大于另一个核。两核间的干涉被大大抑制,在40 ~ 125 eV范围内出现了超连续谱。时频分析和有限初始横向速度的半经典三步模型很好地解释了其物理机制。通过几次谐波的叠加,可以产生持续时间为80 As的孤立阿秒脉冲。
The generation of high-order harmonic and the attosecond pulse of the N-2 molecule with an orthogonally polarized two-color laser field are investigated by the strong-field Lewenstein model. We show that the control of contributions to high-order harmonic generation (HHG) from different nuclei is realized by properly selecting the relative phase. When the relative phase is chosen to be phi= 0.4 pi, the contribution to HHG from one nucleus is much more than that from another. Interference between two nuclei can be suppressed greatly; a supercontinuum spectrum of HHG appears from 40 eV to 125 eV. The underlying physical mechanism is well explained by the time-frequency analysis and the semi-classical three-step model with a finite initial transverse velocity. By superposing several orders of harmonics, an isolated attosecond pulse with a duration of 80 as can be generated.
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