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The Method for Scanning Reshaping the Spectrum of Chirped Laser Pulse Based on the Quadratic Electro-Optic Effects

机译:基于二次光电效应的Chi激光脉冲频谱扫描整形方法

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T A new method for scanning reshaping the spectrum of chirped laser pulse based on quadratic electro-optic effects is proposed. The scanning reshaping scheme with a two-beam interference system is designed and the spectrum reshaping properties are analyed theoretically. For the Gaussian chirped laser pulse with central wavelength λ_0=800nm, nearly flat-topped spectral profiles with wider bandwidth is obtained with the proposed scanning rehsaping method, which is beneficial to compensate for the gain narrowing effect in CPA and OPCPA. Further numerical simulations show that the reshaped spectrum is sensitive to the time-delay and deviation of the voltage applied to the crystal. In order to avoid narrowing or distorting the reshaped spectrum pointing to target, it is necessary to reduce the unfavorable deviations. With the rapid and wide applications of ultra-short laser pulse supported by some latter research results including photo-associative formation of ultra-cold molecules from ultra-cold atoms~[1-3], laser-induced communications~[4], capsule implosions on the National Ignition Facility(NIF)~[5-6], the control of the temporal and spectral profiles of laser pulse is very important and urgently need to be addressed. Generally, the control of the pulse profiles depends on practical applications, ranging from femtosecond and picosecond to nanosecond. For instance, the basic shaping setup is a Fourier transform system for ultra-short laser pulse. The most important element is a spatially patterned mask which modulates the phase or amplitude, or sometimes the polarization after the pulse is decomposed into its constituent spectral components by usually a grating and a lens~[7]. One of the generation techniques of ultra-short laser pulse is the chirped pulse amplifications(CPA), which brings a new era of development for high energy and high peak intensity ultra-short laser pulse, proposed by D. Strcik and G. Mourou from the chirping radar technology in microwave region since 1985~[8]. The other generation technique of ultra-short pulse is the optical parametric chirped pulse amplification(OPCPA) invented by Dubietis et al. in 1992, which combined the respective superiorities of CPA and optical parametric amplification(OPA). However, there are disadvantages for the both technologies such as gain narrowing, gain saturation effects, and even spectrum shift. The first one among the three is the most significant which narrows the spectrum after amplification so that it limits the minimum durations of ultra-short laser pulse. This paper proposed a approach for scanning reshaping the spectrum of chirped laser pulse to compensate for the gain narrowing effect, according to the characteristics of the chirped laser pulse, i.e. the frequency varies with time linearly. The spectral characteristics of the scanning reshaping was analyzed quantitatively. Furthermore, the influence of the time-delay and deviation of the controlling voltage employed on the electro-optic crystal on the reshaped spectrum was also been discussed detailedly.
机译:提出了一种基于二次电光效应的扫描整形laser激光脉冲频谱整形的新方法。设计了具有两光束干涉系统的扫描整形方案,并从理论上分析了频谱整形特性。对于中心波长为λ_0= 800nm的高斯chi激光脉冲,利用所提出的扫描重定形方法可以获得具有较宽带宽的近平顶光谱轮廓,这有利于补偿CPA和OPCPA中的增益变窄效果。进一步的数值模拟表明,重塑后的光谱对施加于晶体的电压的时间延迟和偏差很敏感。为了避免使指向目标的重构光谱变窄或失真,有必要减小不利的偏差。随着超短激光脉冲的快速和广泛应用,后来的一些研究成果支持了这种研究,包括由超冷原子〜[1-3]与光缔合形成超冷分子〜,激光诱导的通信〜[4],胶囊在国家点火装置(NIF)〜[5-6]的内爆中,控制激光脉冲的时间和光谱分布非常重要,迫切需要解决。通常,对脉冲轮廓的控制取决于实际应用,范围从飞秒,皮秒到纳秒。例如,基本的整形设置是用于超短激光脉冲的傅立叶变换系统。最重要的元素是空间图案化的掩模,该掩模可调制相位或幅度,或者有时通过通常由光栅和透镜[7]将脉冲分解成其组成的光谱成分后的极化。 -脉冲放大(CPA)是超短激光脉冲的一种生成技术,它是由D. Strcik和G. Mourou提出的高能量和高峰值强度超短激光脉冲的新发展时代。 1985〜[8]以来微波地区的rp雷达技术。超短脉冲的另一种生成技术是Dubietis等人发明的光学参量chi脉冲放大(OPCPA)。 1992年,它结合了CPA和光学参量放大(OPA)各自的优势。但是,这两种技术都存在诸如增益变窄,增益饱和效应甚至频谱偏移之类的缺点。这三个中的第一个是最重要的,它在放大后使光谱变窄,从而限制了超短激光脉冲的最小持续时间。根据proposed激光脉冲的特性,即频率随时间线性变化,本文提出了一种扫描re激光脉冲频谱的整形方法,以补偿增益变窄的影响。定量分析了扫描整形的光谱特征。此外,还详细讨论了电光晶体的时间延迟和控制电压偏差对整形光谱的影响。

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