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1.
吴先前  黄晨光 《强激光与粒子束》2022,34(1):011003-1-011003-19
随着高功率密度激光技术的快速发展,强激光驱动的爆炸与冲击效应逐渐引起国内外学者的广泛关注。对强激光诱导爆炸与冲击效应研究进展进行了综述,包括强激光诱导爆炸载荷特征与相似律,强激光对材料表面冲击强化处理,强激光冲击诱导材料相变动力学行为,以及利用强激光驱动微弹道冲击等方面的研究进展,并指出了强激光诱导爆炸与冲击效应研究的发展趋势和未来需要解决的关键科学问题。  相似文献   

2.
《新兴的强激光》一书将比较全面系统地介绍自由电子激光、X光激光、化学激光、准分子激光等新兴的强激光技术。本书物理概念准确,原理、技术兼顾,中外结合,文字精练,数据可靠,图文并茂,深入浅出,是新型高功率激光技术的一本入门书。本书不但可以使广大读者对强激光技术的基本原理、关键技术及其相关技术,有一个全貌的、形象化的了解,而且对国内外强激光技术研究工作的现状、动态和发展前景也可以有较深入的了解。本书既注重知识性和科学性,也具有较好的可读性和趣味性,因而也是一本强激光技术方面的高级科普读物。  相似文献   

3.
强激光经5CB液晶传播时会产生非线性自相位调制现象,利用532 nm和1 064 nmCW激光研究了强激光条件下5CB液晶中的激光诱导衍射环现象,并对强激光在5CB液晶中产生自相位调制的现象和机理进行了讨论.当532 nm激光和1 064 nm激光功率密度分别大于10 kW/cm2和300W/cm2时,接收白屏上有较明...  相似文献   

4.
在强激光重元素靶等离子体中,电子是不能完全剥离的,带有未离化束缚电子的原子的形状受强激光或超强激光与它的相互作用要发生变化,从而产生极化电流,势必影响强激光等离子体相互作用,随着激光聚变发展的要求,精密物理的需要,研究束缚电子对受激喇曼散射的影响很有必要。  相似文献   

5.
强激光远场光斑强度分布测量技术   总被引:3,自引:2,他引:1       下载免费PDF全文
准确测量激光远场光斑强度时空分布是分析强激光大气传输效应和评价激光系统性能的有效手段。概述了测量激光光斑强度分布的几种方法及其适用性,重点叙述了基于阵列探测法的强激光远场光斑强度分布测量技术,总结分析了量热阵列法、光电阵列法和量热/光电复合法等三类阵列探测系统应用特点。最后介绍了两种分别用于测量连续波高能激光和重频脉冲激光的光电阵列靶斑仪,系统具有结构紧凑的特点,能够满足运动靶目标上强激光参数测量要求。  相似文献   

6.
强脉冲激光在AZ31B镁合金中诱导冲击波的实验研究   总被引:2,自引:0,他引:2       下载免费PDF全文
为了研究强脉冲激光在镁合金中诱导冲击波的衰减,采用Nd:Glass脉冲激光(1054 nm,23 ns)对AZ31B变形镁合金试样表面进行冲击,并利用响应快、测量范围大的PVDF压电膜传感器以及示波器实时测量了强脉冲激光在镁合金靶中诱导激光冲击波的相对压力.根据冲击波每次在靶材背面反射时,所经过距离的不同得到激光冲击波在镁合金中的衰减规律.结果表明,在激光能量为5J的强脉冲激光作用下,镁合金中冲击波衰减的平均速度为5.83×103 m/s,与镁合金中应力波纵波的传播速度相符;强脉冲激光诱导冲击波在镁合金中是以指数规律衰减的.试验所得分析结果对激光冲击强化镁合金的应用具有重要意义. 关键词: 激光 镁合金 压电膜传感器 衰减规律  相似文献   

7.
本文研究了800nm飞秒强激光场下OCS分子的里德堡态激发过程. 实验不仅观测到强激光场中的中性母体分子的里德堡态激发,而且观测到大量的中性里德堡态碎片. 我们测量了里德堡态激发产率随激光强度及椭偏率的变化,并与强场电离解离进行了比较. 分析表明,飞秒激光场下中性里德堡态碎片的产生与强场多次电离密切相关. 此外,我们还讨论了中性里德堡态碎片对激光椭偏率依赖的内在原因.  相似文献   

8.
满宝元  张杰 《物理》2000,29(5):283-288
超短脉冲强激光与团簇的相互作用已被证明能够产生能量高达MeV量级的高能离子和中子以及非常强的X射线辐射。广阔好原子团簇在超短脉冲强激光场的作用下的加热、电离和膨胀等机制,对这种相互作用的深入研究可能会对激光核聚变和X射线激光等应用领域产生重大影响。  相似文献   

9.
强激光场下原子分子的多光子电离和隧道电离是极端条件下的量子现象,也是强场光物理中基本的动力学过程.测量原子分子在强激光场中的超快动力学对探索微观粒子内部结构和相互作用有重要意义.本文简述强场光电离中的基本概念和现象,并介绍强激光与原子分子相互作用研究中的重要仪器——冷靶反冲离子动量成像谱仪(COLT-RIMS),最后展...  相似文献   

10.
 介绍了激光打靶产生短脉冲强X光辐射的方法,给出了打钠靶的数值模拟结果。 数值研究短脉冲强钠X光泵浦氖激光介质的X光激光,通过在氖中加氢的办法降低了电子温 度,有效地提高了激光增益。研究了短脉冲强X光泵浦的高增益光电离三体复合X光激光机 制,提出了在大中型激光器上开展这种X光激光研究的想法。  相似文献   

11.
1 Introduction  HighorderharmonicemissionofgasatominteractionwithintenselaserfieldisapromisingmethodtoproduceacoherentultravioletandsoftXraysource.Sincethefirstexperimentalobservationofthehighorderharmonicemissionofraregasesexposedtointenselase…  相似文献   

12.
Here, soft X‐ray synchrotron radiation transmitted through microchannel plates is studied experimentally. Fine structures of reflection and XANES Si L‐edge spectra detected on the exit of silicon glass microcapillary structures under conditions of total X‐ray reflection are presented and analyzed. The phenomenon of the interaction of channeling radiation with unoccupied electronic states and propagation of X‐ray fluorescence excited in the microchannels is revealed. Investigations of the interaction of monochromatic radiation with the inner‐shell capillary surface and propagation of fluorescence radiation through hollow glass capillary waveguides contribute to the development of novel X‐ray focusing devices in the future.  相似文献   

13.
杨家敏  丁耀南 《光学学报》1998,18(4):26-430
利用星光Ⅱ激光装置钕玻璃三倍频激光辐照金箔靶,实验研究了金箔靶背侧发射的X光能谱,时间过程和秀过激光能量。结果表明:金箔背侧发的X光可以作为一种较干净的强X光射源。  相似文献   

14.
利用软X射线大面积透射光栅谱仪,对超短强激光脉冲辐照下玻璃微毛细管靶的软X射线发射特性进行了研究。测得了不同的激光能量下、不同长度(3mm、6mm、9mm)的微毛细管的软X射线发射谱,并观察到随着微毛细管长度的增加,X射线发射强度增强。  相似文献   

15.
用网格衰减膜相对标定SIOFM─5FW软X光底片   总被引:1,自引:0,他引:1  
点聚焦激光等离子体发出的X射线经晶体色散形成均匀的单色X射线源,在此基础上,用单层网格作为衰减膜,得到未经衰减和经过衰减的X射线谱,对无保护膜SIOFM5FW软X光底片作了试验性的相对标定,得到了0.91nm波长的特性曲线  相似文献   

16.
The technical implementation of a multi‐MHz data acquisition scheme for laser–X‐ray pump–probe experiments with pulse limited temporal resolution (100 ps) is presented. Such techniques are very attractive to benefit from the high‐repetition rates of X‐ray pulses delivered from advanced synchrotron radiation sources. Exploiting a synchronized 3.9 MHz laser excitation source, experiments in 60‐bunch mode (7.8 MHz) at beamline P01 of the PETRA III storage ring are performed. Hereby molecular systems in liquid solutions are excited by the pulsed laser source and the total X‐ray fluorescence yield (TFY) from the sample is recorded using silicon avalanche photodiode detectors (APDs). The subsequent digitizer card samples the APD signal traces in 0.5 ns steps with 12‐bit resolution. These traces are then processed to deliver an integrated value for each recorded single X‐ray pulse intensity and sorted into bins according to whether the laser excited the sample or not. For each subgroup the recorded single‐shot values are averaged over ~107 pulses to deliver a mean TFY value with its standard error for each data point, e.g. at a given X‐ray probe energy. The sensitivity reaches down to the shot‐noise limit, and signal‐to‐noise ratios approaching 1000 are achievable in only a few seconds collection time per data point. The dynamic range covers 100 photons pulse?1 and is only technically limited by the utilized APD.  相似文献   

17.
Dynamic X‐ray studies can reach temporal resolutions limited by only the X‐ray pulse duration if the detector is fast enough to segregate synchrotron pulses. An analog integrating pixel array detector with in‐pixel storage and temporal resolution of around 150 ns, sufficient to isolate pulses, is presented. Analog integration minimizes count‐rate limitations and in‐pixel storage captures successive pulses. Fundamental tests of noise and linearity as well as high‐speed laser measurements are shown. The detector resolved individual bunch trains at the Cornell High Energy Synchrotron Source at levels of up to 3.7 × 103 X‐rays per pixel per train. When applied to turn‐by‐turn X‐ray beam characterization, single‐shot intensity measurements were made with a repeatability of 0.4% and horizontal oscillations of the positron cloud were detected.  相似文献   

18.
The implementation of a laser pump/X‐ray probe scheme for performing picosecond‐resolution X‐ray diffraction at the 1W2B wiggler beamline at Beijing Synchrotron Radiation Facility is reported. With the hybrid fill pattern in top‐up mode, a pixel array X‐ray detector was optimized to gate out the signal from the singlet bunch with interval 85 ns from the bunch train. The singlet pulse intensity is ~2.5 × 106 photons pulse?1 at 10 keV. The laser pulse is synchronized to this singlet bunch at a 1 kHz repetition rate. A polycapillary X‐ray lens was used for secondary focusing to obtain a 72 µm (FWHM) X‐ray spot. Transient photo‐induced strain in BiFeO3 film was observed at a ~150 ps time resolution for demonstration.  相似文献   

19.
 在星光激光装置上, 使用X射线多层膜反射镜、铝滤片及X射线CCD探测器组成高灵敏度空间分辨探测系统, 对用预脉冲技术产生的类Ne钛单线 (J=0-1, 3p-3s跃迁)软X射线激光输出特性进行了测量。由实验得到了类Ne钛X 射线激光束近场与距靶端32mm处(准远场)强度的空间分布, 给出了该激光束在近场强度最大区域的空间尺度(FWHM)约为72μm×31μm, 以及在垂直靶面与平行靶面方向的束发散角分别约为4mrad与9mrad。  相似文献   

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