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1.
纳秒激光在铜靶材中诱导冲击波的实验研究   总被引:1,自引:0,他引:1       下载免费PDF全文
王绩勋  高勋  宋超  林景全 《物理学报》2015,64(4):45204-045204
基于聚偏二氟乙烯压电传感器, 对铜靶材中纳秒激光脉冲诱导的冲击波传播过程进行了实验研究, 给出了铜靶材内冲击压强随激光脉冲能量和靶材厚度的变化规律. 实验结果表明: 500 mJ激光脉冲能量作用到2 mm厚的铜靶材产生的冲击压强达到2.1 MPa; 激光脉冲能量从200 mJ 增加到500 mJ, 在铜靶材厚度为2和4 mm条件下, 冲击压强分别增加了162%和231%; 而当铜靶材厚度从2 mm增加到6 mm时, 在400和500 mJ激光脉冲能量作用下, 铜靶材内冲击压强分别降低了32%和49%.  相似文献   

2.
利用Nd:YAG激光(波长1 064 nm,脉宽10 ns)烧蚀金属Cu靶获得等离子体 .改变激光脉冲能量,观测到Cu的原子谱线和离子谱线随激光脉冲能量有不同的变化关系, 但都在330 mJ/pulse时,谱线强度达到最大,随后在330 mJ~370 mJ/pulse间出现一小平台 ,能量继续增加,各谱线强度减小.同时,使用烧蚀Cu靶产生的五条原子谱线(465.11 nm,5 10.55 nm,515.32 nm,521.82 nm,529.25 nm)的相对强度,在局部热力学平衡近似下,利用B oltzmann图的最小二乘法拟合,测定了不同激光能量下Cu等离子体的电子温度.随激光能量的增加,电子温度近似单调地从1.02×104 K上升到1.46×104 K后,反而有所下降.  相似文献   

3.
应用多光子非线性Compton散射理论,研究了Compton散射下的强激光等离子体冲击波对固体的热烧蚀效应,给出了冲击波功率密度与靶材熔化温度及沸腾温度与加热时间的表达式,得到了冲击波照射靶材烧蚀孔的最佳实验条件。结果表明:固体的生热率提高,温度分布发生变化,作用点达到熔化和沸腾温度所需时间和功率比无散射时小。当冲击波能量为250J,到靶面的距离为70~80mm时,对靶材烧蚀孔的效果较好。当时间为1.2~3.6ms,到靶面的距离为28~80mm时,烧蚀效果较好;当能量密度为400~2800J•cm-2时,烧蚀深度成较差的线性增加,功率密度与烧蚀斑尺寸近乎成反比。  相似文献   

4.
采用波长为355 nm的纳秒紫外重复脉冲激光对单晶硅片进行了盲孔加工实验, 观测了随脉冲增加激光烧蚀硅片的外观形貌和盲孔孔深、孔径的变化规律, 并对紫外激光辐照硅片的热力学过程进行了分析. 研究结果表明:紫外激光加工硅盲孔是基于热、力效应共同作用的结果, 热效应会使得硅材料熔化、气化甚至发生电离产生激光等离子体,为材料的去除提供条件;激光等离子体冲击波以及高温气态物向外膨胀会对熔化材料产生压力致使其向外喷射,为重复脉冲的进一步烧蚀提供了条件;力效应主要沿着激光传输的方向,垂直于硅表面,使得去除部位主要集中在孔的深度方向,达到较高的孔径比,实验观察孔径比可达8:1;此外,激光等离子体的产生也阻止了激光对靶面的作用,加之随孔深的增加激光发生散焦,使得烧蚀深度有一定的限制,实验观察烧蚀脉冲个数在前100个时加工效率较高.  相似文献   

5.
利用时间分辨阴影成像技术进行飞秒激光烧蚀金属表面研究可以直观获取飞秒激光烧蚀金属表面产生冲击波膨胀过程的图像。通过对比飞秒激光烧蚀金属铝、铜、铁靶表面的冲击波膨胀形式发现:金属铜、铁表面的冲击波均以球面波形式传播;由于受到烧蚀物质喷溅的影响,铝靶表面竖直方向的冲击波传播形式由球面波转化为柱面波。  相似文献   

6.
张彪  高玮  杨照金  杨鸿儒 《应用光学》2009,30(4):703-706
为满足一些武器装备对激光系统小型化及输出激光光斑均匀性较高的要求,通过设计LD侧面对称半环状泵浦的泵浦方式,使得输出的激光光斑形状基本为圆形,激光光斑的均匀性有了较大提高.采用凹面全反射镜补偿热效应以及设计紧凑激光谐振腔型,在注入电流60 A、频率为20 Hz时,得到平均单脉冲能量为96 mJ (脉冲能量波动小于6%)、脉宽为10 ns、发散角为3 mrad的近似圆形激光输出,激光系统在高温50℃时工作稳定.  相似文献   

7.
张璐  杨家敏 《物理学报》2012,61(4):45203-045203
X射线烧蚀泡沫-固体靶时界面失配会使得泡沫与固体靶中压力增加, 这一现象可用于研究高压下物质的状态方程. 本文以CH泡沫-Al固体靶为例, 研究了X射线烧蚀双层靶时的增压现象. 提出仅当泡沫中有冲击波产生时, 在固体靶中才会有增压现象出现. 文中基于冲击波强波近似, 理论分析了冲击波过界面情况与冲击波、稀疏波作用过程, 得到增压倍数与材料密度, 多方气体指数的近似表达式. 同时表明固体靶中增压产生的冲击波为高压脉冲, 会被紧跟热波的稀疏波追赶并稀疏. MULTI一维计算结果验证了该结论.  相似文献   

8.
飞秒激光在铝膜中驱动冲击波的特性   总被引:1,自引:0,他引:1       下载免费PDF全文
为探索研究飞秒激光在材料中驱动冲击波的相关特性,采用激光脉冲频域干涉测试技术对脉冲宽度35fs、脉冲能量0.7mJ、功率密度1014W/cm2量级的飞秒激光脉冲在200nm厚铝膜中驱动冲击波的过程进行了实验测量。通过测量冲击波在铝膜中的渡越时间,获得激光脉冲在铝材料中驱动的冲击波平均速度约为6km/s;通过对不同时刻铝膜自由面频域干涉场测量结果的分析,获得铝材料自由表面速度达1km/s,根据平面冲击波的关系,推算其冲击压强达到9GPa。  相似文献   

9.
罗乐乐  窦志国  叶继飞 《物理学报》2018,67(18):187901-187901
选择含能聚合物聚叠氮缩水甘油醚(GAP)作为激光烧蚀微推力器的工质,分析了红外染料掺杂对激光烧蚀GAP工质推进性能的影响.通过对比掺杂红外染料GAP在不同激光功率密度、掺杂浓度、靶材厚度和激光烧蚀模式下的推进性能数据和烧蚀羽流,初步探索了掺杂红外染料GAP工质的推进性能优化方式.实验结果表明:透射式激光烧蚀模式下,激光能量的指数衰减特性和掺杂红外染料GAP的强黏性使得烧蚀羽流中易存在未充分烧蚀的工质; GAP的推进性能受红外染料掺杂浓度和靶材厚度的综合影响,当靶材厚度与激光吸收深度接近时,靶材充分吸收激光能量使中心烧蚀区达到化学能释放的温度阈值,同时沿激光传播方向未充分烧蚀的质量最少,此时推进性能达到最优值.反射式下掺杂红外染料的聚合物的激光烧蚀过程遵循"先吸收激光能量先喷射"的规律,工质分解充分,推进性能优于透射式.  相似文献   

10.
空气中激光等离子体冲击波的传输特性研究   总被引:1,自引:0,他引:1       下载免费PDF全文
根据球形对称冲击波在自由空间中传播的约束条件,提出了空气中激光等离子体冲击波在中远场的传播公式.并用探针式超声换能器实测了能量为10-110mJ、脉宽为15ns、波长为106μm的Nd∶YAG激光作用于铝靶表面产生的等离子体空气冲击波,用此公式计算的结果与实验数据符合得很好 关键词:  相似文献   

11.
Aluminum ablation by multiple femtosecond laser pulses is investigated via time-resolved shadowgraphs and scanning electron microscope(SEM) images of the ablation spot. The spatial distribution of the ejected material and the radius of the shock wave generated during the ablation are found to vary with the increase in the number of pulses. In the initial two pulses, nearly concentric and semicircular stripes within the shock wave front are observed, unlike in subsequent pulses. Ablation by multiple femtosecond pulses exhibits different characteristics compared with the case induced by single femtosecond pulse because of the changes to the aluminum target surface induced by the preceding pulses.  相似文献   

12.
Femtosecond(fs) pulse laser ablation of silicon targets in air and in vacuum is investigated using a timeresolved shadowgraphic method. The observed dynamic process of the fs laser ablation of silicon in air is significantly different from that in vacuum. Similar to the ablation of metallic targets,while the shock wave front and a series of nearly concentric and semicircular stripes,as well as the contact front,are clearly identifiable in the process of ablation under 1×10 5 Pa,these phenomena are no longer observed when the ablation takes place in vacuum. Although the ambient air around the target strongly affects the evolution of the ablation plume,the three rounds of material ejection clearly observed in the shadowgraphs of fs laser ablation in standard air can also be distinguished in the process of ablation in vacuum. It is proven that the three rounds of material ejection are caused by different ablation mechanisms.  相似文献   

13.
In this investigation, we used high-speed shadow photography to observe fast optodynamic phenomena such as shock waves and the ablation of flat metal surfaces. These phenomena were induced in air by a Q-switched Nd:YAG laser (λ = 1,064 nm) with a pulse duration of 4 ns and an excitation pulse energy between 10 and 55 mJ. For a good spatial resolution of the shadowgraphs, we used short illumination pulses (30 ps) from a frequency-doubled Nd:YAG laser (λ = 532 nm). Using the shadowgraphs of the shock wave expansion into a half-space, we measured the optodynamic energy conversion efficiency, defined as the ratio between the mechanical energy of the shock wave and the excitation pulse energy. This efficiency increases with an increasing excitation pulse energy. We also present the characteristic shadowgraphs of the ablation of a black-painted metal surface, where the macroscopic material particles are clearly visible. They follow the shock wave and eventually overtake it. As a result, the shape of the shock wave, which normally expands concentrically into the half-space, has an altered form. The presented results reveal the phenomenon of the laser ablation of coated metal surfaces.  相似文献   

14.
The influence of air pressure on mechanical effect of laser plasma shock wave in a vacuum chamber produced by a Nd:YAG laser has been studied. The laser pulses with pulse width of 10ns and pulse energy of about 320mJ at 1.06$\mu $m wavelength is focused on the aluminium target mounted on a ballistic pendulum, and the air pressure in the chamber changes from $2.8\times 10^{3}$ to 1.01$\times $10$^{5 }$Pa. The experimental results show that the impulse coupling coefficient changes as the air pressure and the distance of the target from focus change. The mechanical effects of the plasma shock wave on the target are analysed at different distances from focus and the air pressure.  相似文献   

15.
应用高速纹影系统记录激光束辐照在Ly12铝靶时所产生的汽化羽扩张、空气爆炸波、熔融物质喷溅以及穿靶等现象.并由扫描摄影记录的轨迹图测出汽化羽的扩张速度为150~190m/s,空气冲击波速度为450~500m/s,靶表面高压蒸汽速度为5~7.8km/s。  相似文献   

16.
任欢  王俊波  邱荣  周强  刘浩  马平 《强激光与粒子束》2012,24(12):2787-2790
利用基于Pump-probe系统的超快时间分辨阴影图的方法,研究了空气中飞秒激光烧蚀单晶硅的动力学过程。实验采用脉宽为50 fs、平均能量密度约35 J/cm2的单脉冲激光烧蚀单晶硅,获取飞秒激光烧蚀单晶硅过程中等离子体和冲击波的形成和发展过程的时间分辨阴影图。实验结果表明:飞秒激光烧蚀单晶硅导致其表面物质喷发的过程是不连续的,分为明显的两次喷发过程。这表明飞秒激光与单晶硅作用的过程中,在不同的时间段可能由不同的机制主导,在前期可能是多光子电离为主,在后期可能是由多光子效应和雪崩效应共同作用。研究还发现,延迟时间较长时,冲击波形状发生畸变。  相似文献   

17.
The propagation of a plasma shock wave generated from an Al target surface ablated by a nanosecond Nd:YAG laser operating at 355 nm in air is investigated at the different focusing positions of the laser beam by using a time-resolved shadowgraph imaging technique. The results show that in the case of a target surface set at the off-focus position, the condition of the focal point behind or in front of the target surface greatly influences the evolution of an Al plasma shock wave, and an ionization channel forms in the case of the focal point set in front of the target surface. Moreover, it is found that the shadowgraph with the evolution time around 100 ns shows that a protrusion appears at the front tip of the shock wave if the focal point is at the target surface. In addition, the calculated results of the expanding velocity of the shock wave front, the mass density, and pressure just behind the shock wave front are presented based on the shadowgraphs.  相似文献   

18.
K P J Reddy 《Pramana》1996,46(2):153-159
The aerodynamics of the blast wave produced by laser ablation is studied using the piston analogy. The unsteady one-dimensional gasdynamic equations governing the flow are solved under assumption of self-similarity. The solutions are utilized to obtain analytical expressions for the velocity, density, pressure and temperature distributions. The results predict all the experimentally observed features of the laser produced blast waves.  相似文献   

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