Action of a femtosecond laser pulse on thin metal film supported by glass substrate

被引:0
|
作者
Shepelev, V. V. [1 ,2 ]
Inogamov, N. A. [2 ,3 ]
Fortoval, S., V [1 ]
Danilov, P. A. [4 ]
Kudryashov, S., I [4 ]
Kuchmizhak, A. A. [5 ,6 ]
Vitrik, O. B. [5 ,6 ]
机构
[1] Russian Acad Sci, Inst Comp Aided Design, 19-18 Vtoraya Brestskaya St, Moscow 123056, Russia
[2] Russian Acad Sci, Landau Inst Theoret Phys, 1a Akad Semenova Ave, Chernogolovka 142432, Moscow Region, Russia
[3] Dukhov Res Inst Automat VNIIA, 22 Sushchevskaya, Moscow 127055, Russia
[4] Russian Acad Sci, Lebedev Phys Inst, 53 Leninsky Ave, Moscow 119991, Russia
[5] Russian Acad Sci, Inst Automat & Control Proc, Far Eastern Branch, 5 Radio St, Vladivostok 690041, Primorsky Krai, Russia
[6] Far Eastern Fed Univ, Sch Nat Sci, 8 Sukhanova St, Vladivostok 690041, Primorsky Krai, Russia
基金
俄罗斯基础研究基金会;
关键词
GENERATION; ABLATION; NANOJETS;
D O I
10.1088/1742-6596/1128/1/012092
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Numerous papers are devoted to the problem of irradiating thin films on the substrate for surface nano-modification. But all of them concern the dynamics of the dynamics, paying almost no attention to substrate just as object of the first shockwave absorption. A different point of view with an emphasis on the dynamics of a substrate is presented. Under powerful laser action upon a thin metal film a hole arises. Its radius depends on the absorbed laser energy. Experimental results, quantitative theoretical model and numerical research are presented and show that the hole formation is influenced by propagation of the shock wave in the substrate, but not in the film itself. Four stages are considered. (i) Shockwave generation in a support because of an impact of a contact. (ii) Transition from one-dimensional to two-dimensional propagation of the shockwave. (iii) Lateral propagation of the shockwave along a film-support contact. And (iv) calculating pressure in the compressed layer behind the decaying shockwave. This positive pressure acting from substrate on the film accelerates the film in direction to vacuum. Above some threshold, velocity of accelerated film is enough to separate the film from support. In these cases the circle of separation is significantly wider than the focal laser spot on film surface.
引用
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页数:8
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