Use of KD*P crystals for non-degenerated broadband optical parametric chirped pulse amplification in petawatt lasers

G. Freidman, N. Andreev, V. Bespalov, V. Bredikhin, V. Ginzburg, E. Katin, A. Korytin, E. Khazanov, V. Lozhkarev, O. Palashov, A. Sergeev, I. Yakovlev, S. Garanin, N. Rukavishnikov, S. Sukharev
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引用次数: 6

Abstract

The problem of creating optical parametric amplifiers of femtosecond pulses up to the multiterawatt level was fiist discussed in [l, 21. In these papers, as well as in subsequent studies [3-91, only nonlinear elements made from KDP crystals, whose aperture can be as great as 30cm, were considered as nonlinear elements for final cascades of optical parametric amplifiers (OPAs). The most promising pump source is the second harmonic of a Nd:glass laser with a wavelength of 3L3=527nm. At this pumping, the KDP crystal has two serious disadvantages: it absorbs greatly at wavelengths higher than 1200nm and has maximal gain bandwidth (1000-1200~m~[l~]) at the wavelength of signal 1050-1 1 OOnm, i.e., at degenerated (or nearly degenerated) phasematching. In this wavelength range, however, it is difficult to create light sources with pulse duration of less than 50fs.
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KD*P晶体用于非简并宽带光参量啁啾脉冲放大的百瓦激光器
在[1,21]中首先讨论了创建多太瓦级飞秒脉冲光参量放大器的问题。在这些论文以及随后的研究[3-91]中,只有孔径可达30cm的KDP晶体制成的非线性元件才被认为是光学参数放大器(OPAs)最终级联的非线性元件。最有希望的泵浦源是波长为3L3=527nm的Nd:玻璃激光器的二次谐波。在这种泵浦下,KDP晶体有两个严重的缺点:它在高于1200nm的波长处吸收很大,并且在信号波长1050-1 OOnm处,即在退化(或近退化)相位匹配处具有最大增益带宽(1000-1200~m~[l~])。然而,在这个波长范围内,很难制造出脉冲持续时间小于50fs的光源。
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