Abstract

In order to accurately analyze the broadband pulsed amplification performances of the domestic picosecond petawatt laser system, which uses large aperture N<sub>31</sub> or N<sub>41</sub> neodymium glass as gain medium, the broadband pulsed amplification model is improved by introducing the actual stimulated emission cross section (SECS) of neodymium glass. Comparing with the SECS under Gaussian approximation, the amplified pulsed spectrum gain narrowing effect with different SECSs are analyzed. It is found that in the actual SECS of N<sub>31</sub> neodymium glass laser, the gain-narrowing effect is enhanced, the output energy decreases, gain’s saturation effect weakens, system’s accumulated <i>B</i> integral augments, but the laser system turns insensitive to the center wavelength simultaneously. Based on the Shenguang II high energy picosecond petawatt laser system which uses N<sub>31</sub> neodymium glass, the spectral shape, center wavelength, and energy stability of amplified output pulse are simulated by using different SECSs. It is shown that the super-Gaussian spectral shape narrows more greatly than Gaussian spectral shape, the spectrum bandwidth narrows from 10 to about 3 nm with gain larger than 10<sup>7</sup>, and the accumulated <i>B</i> integral increases to 1.7. Additionally, the gain-narrowing effect makes the output spectrum (with 1054 nm of center wavelength) less affected by changing the inputted center wavelength from 1052 to 1056 nm, and the gain saturation effect can improve output energy stability to less than 2% (root mean square (RMS)) with about 3% (RMS) inputted energy stability, which are beneficial to the subsequent pulse compression and physical experiment. Based on the above analysis, a broadband pulsed amplified experiment is conducted by using Shenguang II petawatt laser system, the injected seed is about 10 nm (full width at half maximum (FWHM)) with 5 order super Gaussian shape at 1054-nm center wavelength, and 1.2 mJ with 3% (RMS) energy stability from optical parametric chirped pulse amplification. The amplified pulse with 1900 J at 1054.2 nm (3 nm FWHM) and stability < 2% (shot to shot) is achieved, and the spectral shapes and bandwidths after bar and disk amplifiers are measured, which are consistent with theoretical analysis results. The results can provide a necessary reference for constructing high energy broadband laser system and improving its performances in the future.

Highlights

  • The compared numerical results of spectrum and upper state population after 70 (a), (b) and 350 (c), (d) amplifier, which influenced by different stimulated emission cross section (SECS)

  • Input a 1.2 mJ, 5 ns, 10 nm broadband seed, and the main simulation parameters after bar and disk amplifier, which influenced by different SECSs

  • 在理论分析的基础上, 利用注入的 10 nm (FWHM) 超高斯形状 、 1054 nm 中 心 波 长 、 3% (RMS) 能量稳定性的参量放大种子, 实现了 1900 J、 中心波长 1054.2 nm、谱宽 3 nm 的输出, 发次能量 稳定性 < 2%, 与理论分析结果一致

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Summary

Introduction

啁啾脉冲放大激光系统中展宽器色散的解析算法 Analytical algorithem of stretcher dispersion in chirp pulse amplification laser system 物理学报. 在此基础上, 利用神 光 II 皮秒拍瓦激光系统开展了实验研究, 对于光 参量啁啾脉冲放大注入的 10 nm (FWHM) 超高 斯形状、1054 nm 中心波长、3% (RMS) 能量稳定 性种子, 实现了 1900 J、中心波长 1054.2 nm、谱 宽 3 nm 的输出, 发次间能量稳定性 < 2%, 与采 用实际 SECS 理论分析结果一致. 常数 K = εcσ0 (λ) ∆ωa , 其中 σ0 (λ)为增益介质的 SECS, 2∗ 为饱和因子 (取值在 1—2 之间); ħ 为普朗克常数; I (z, t)为光强.

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