共查询到19条相似文献,搜索用时 109 毫秒
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由于独特的优点和广泛的应用前景,X射线激光的研究受到了很大的重视。从一开始,这类研究就是以大型激光器作为驱动源进行的,尽管取得了很大的进展,但是由于对驱动源的要求很高,使得X射线激光自身的发展和应用受到了一定的限制。在这个背景下,如何利用尺寸更小、成本更低、更容易获得的方式来驱动X射线激光成为一个重要的研究目标。迄今为止,已经发展出了毛细管放电、高次谐波、超短超强激光驱动X射线激光等多种方式。特别的,随着近些年来皮秒乃至飞秒超短超强激光技术的发展,使得利用超短超强激光驱动瞬态X射线激光成为X射线激光小型化的一个重要发展方向。 相似文献
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在1.2×1013W·cm-2低功率密度下,对基频激光预主短脉冲驱动类镍银X光激光机理进行了数值模拟和理论分析。证实了在靶长23 mm范围内X光激光都能获得有效放大,取得了和实验相符合的结果。考虑了单柱面镜线聚焦沿靶长度方向功率密度的非均匀性对X光激光放大的影响,采用弯曲靶能有效克服折射以及单柱面镜线聚焦功率密度非均匀带来的不利影响。理论模拟给出的类镍银X光激光的出光下限泵浦功率密度也与实验符合得很好。理论模拟还表明,采用1%左右的预脉冲强度并对预主脉冲时间间隔进行优化,X光激光的输出能量和能量转换效率将获得大幅度提高。 相似文献
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利用脉宽约为50ps的类镍银139nm软X射线激光作为探针,探测由脉宽80ps的驱动激光打C8H8靶产生的等离子体在1ns后的电子密度分布信息,获得了清晰的莫尔条纹图像.对结果的处理,给出了峰值电子密度为11×1021cm-3,并对在靶面附近莫尔条纹的消失现象作了初步解释
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软X射线激光探针 莫尔条纹 等离子体电子密度 相似文献
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介绍了一种利用光电摄谱法和条纹管相结合测量ps级时间分辨超快高能脉冲激光光谱的方法。论述了条纹相机工作原理和平面衍射光栅的分光原理,分析指出利用介绍的装置,可以实现波长300 nm ~1 600 nm、脉宽>2 ps超快高能脉冲激光的光谱测量。采用1 054 nm超快高能脉冲激光器,实验得到了条纹像,对条纹像进行数据处理后得到测量光谱曲线,通过能量标定后,得到了超快高能脉冲激光器实际光谱曲线,验证了ps级时间分辨超快高能脉冲激光光谱方法。讨论了系统中耦合透镜组对光谱测量和光纤色散角对条纹图像的影响,论述了ps级时间分辨超快高能脉冲激光光谱的作用。随着条纹管制造技术的飞速发展,该方法可用于fs级激光光谱的测量。 相似文献
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V. S. Belyaev D. V. Kovkov A. P. Matafonov G. F. Karabadzhak G. G. Raikunov A. Ya. Faenov S. A. Pikuz Jr. I. Yu. Skobelev T. A. Pikuz D. A. Fokin V. E. Fortov G. N. Ignat’ev S. V. Kapitanov P. S. Krapiva K. E. Korotkov 《JETP Letters》2013,97(12):681-685
It is proposed to use a high rate of collisional ionization in a superdense laser plasma to generate incoherent femtosecond X-ray pulses. The calculations indicate that the use of picosecond laser pulses with a contrast of about 1010 will allow the generation of an X-ray pulse with a duration of about 10 fs. The adequacy of the proposed model of the excitation of linear X-ray radiation from the plasma has been tested in the experiments with a picosecond laser of a moderately high contrast. 相似文献
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A robust, self-starting picosecond pulse source based on ytterbium (Yb3+) doped fiber laser is described. Utilizing a chirped-fiber-Bragg-grating (C-FBG) for dispersion control, solitary mode-locking is obtained without bulk dispersion compensation elements. A semiconductor saturable absorber (SESAM) is used for stable self-starting. 3.6 ps pulses are produced, with 45 MHz basic repetition-rate and mW scale average output power at 1060 nm. Detailed numerical simulations based on the modified nonlinear Schrödinger equation agree well with the experimental results and are used as a design tool for the solitary mode-locked picosecond laser. The presented design can be simply employed in an all-fiber environmentally-stable system. 相似文献
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In order to realize the qualitative control of the laser-induced changes trend and the quantitative control of the laser-induced changes range in titanium upon laser irradiation with different pulse duration, comparative ablation experiments by femtosecond, picosecond and millisecond pulsed lasers were carried out on titanium in this study. Then the final surface morphology, aspect ratio, chemical composition and microstructural state of the ablated titanium were analyzed by laser scanning confocal microscopy, X-ray photoelectron spectroscopy and transmission electron microscopy, respectively. The dependency of the morphology, size, composition and microstructure of ablated titanium on laser pulse duration variation were emphatically discussed. It is found that, as the laser pulse duration increases from femtosecond to millisecond scale, surface morphology quality of ablated titanium gets worse, aspect ratio of microgroove decreases, proportion of titanium oxides in final ablation products becomes larger and the microstructural state of ablated titanium has a higher amorphization degree, which can be attributed to the decreased laser intensity per pulse and enhanced heat conduction effect in titanium with the pulse duration increasing. 相似文献
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Spectral and temporal measurements undertaken on a single picosecond laser pulse from a flash lamp pumped, cavity dumped, active/passive mode-locked Nd:YAG laser are presented in this paper. Optimization of several parameters of the resonator cavity produced a single pulse with 0.7 mJ energy and 102 contrast. The pulse duration was variable from 24 to 120 ps by using intra-cavity etalons of different thicknesses. The pulse width and spectrum of the pulse were simultaneously measured using a second harmonic autocorrelator and a spectrometer. The time bandwidth product was 0.445, which is close to theoretical limit for a bandwidth limited pulse. 相似文献
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Analysis of tunable picosecond pulse generation from a distributed feedback Ti:sapphire laser 下载免费PDF全文
A distributed feedback Ti:sapphire laser (DFTL) pumped by a 532nm Q-switched pulse is proposed for the generation of tunable picosecond pulses. With coupled rate equation model, the temporal characteristics of DFTL are obtained. The numerical solutions show that the DFTL pulse with a 50-ps pulse duration and as much as 3.SmJ pulse energy can be obtained under 40-m J, 5-ns pulse pumping. The dependence of output pulse width on the laser crystal‘s length, pumping pulse duration, and pumping rate is also discussed in detail. 相似文献
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Ke Zhang Simian Li Guangfei Liang Huan Huang Yang Wang Tianshu Lai Yiqun Wu 《Physica B: Condensed Matter》2012,407(13):2447-2450
The crystallization dynamics of as-deposited amorphous Ge2Sb2Te5 films induced by nano- and picosecond single laser pulse irradiation is studied using in situ reflectivity measurements. Compared with nanosecond laser pulse, the typical recalescence phenomenon did not appear during the picosecond laser pulse-induced crystallization processes when the pulse fluence gradually increased from crystallization to ablation threshold. The absence of melting and recalescence phenomenon significantly decreased the crystallization time from hundreds to a few tens of nanoseconds. The role of pulse duration time scale on the crystallization process is qualitatively analyzed. 相似文献
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对SiO2和ZnS这两种常用的红外光学材料在红外短脉冲激光辐照下的热损伤特性进行了研究,分析了相同激光辐照条件下两种材料的热效应,另外也针对同种材料不同辐照条件下的热效应进行比较。分析结果表明:红外激光作用下,SiO2材料的表面温升快于ZnS材料,而在材料内部,则后者快于前者。脉冲辐照结束时SiO2材料的表面峰值温度高于ZnS材料,但ZnS材料产生温升的深度大于SiO2材料。由于能量更为集中,材料在皮秒激光作用下温升高于纳秒激光作用下的温升。若材料的峰值温度达到熔点,则激光的单脉冲能量随脉冲宽度的减小呈非线性减小趋势,且变化率越来越大。 相似文献