Phase change mechanisms during femtosecond laser pulse train ablation of nickel thin films

2009 ◽  
Vol 106 (6) ◽  
pp. 064906 ◽  
Author(s):  
Xin Li ◽  
Lan Jiang ◽  
Hai-Lung Tsai
Author(s):  
Jing Huang ◽  
Yuwen Zhang ◽  
J. K. Chen ◽  
Mo Yang

Ultrashort laser pulses can be generated in the form of a pulse train. In this paper, the ultrafast phase change processes of a 1-μm free-standing gold film irradiated by femtosecond laser pulse trains are simulated numerically. A two-temperature model coupled with interface tracking method is developed to describe the ultrafast melting, vaporization and resolidification processes. To deal with the large span in time scale, variable time steps are adopted. A laser pulse train consists of several pulse bursts with a repetition rate of 0.5∼1 MHz. Each pulse burst contains 3∼10 pulses with an interval of 50 ps ∼ 10 ns. The simulation results show that with such a configuration, to achieve the same melting depth, the maximum temperature in the film decreases significantly in comparison to that of a single pulse. Although the total energy depositing on the film will be lifted, more energy will be transferred into the deeper part, instead of accumulating in the sub-surface layer. This leads to lower temperature and temperature gradient, which is favorable in laser sintering and laser machining.


2010 ◽  
Vol 133 (3) ◽  
Author(s):  
Jing Huang ◽  
Yuwen Zhang ◽  
J. K. Chen ◽  
Mo Yang

Ultrashort laser pulses can be generated in the form of a pulse train. In this paper, the ultrafast phase change processes of a 1 μm free-standing gold film irradiated by femtosecond laser pulse trains are simulated numerically. A two-temperature model coupled with interface tracking method is developed to describe the ultrafast melting, vaporization, and resolidification processes. To deal with the large span in time scale, variable time steps are adopted. A laser pulse train consists of several pulse bursts with a repetition rate of 0.5–1 MHz. Each pulse burst contains 3–10 pulses with an interval of 50 ps–10 ns. The simulation results show that with such configuration, to achieve the same melting depth, the maximum temperature in the film decreases significantly in comparison to that of a single pulse. Although the total energy depositing on the film will be lifted, more energy will be transferred into the deeper part, instead of accumulating in the subsurface layer. This leads to lower temperature and temperature gradient, which is favorable in laser sintering and laser machining.


2014 ◽  
Vol 47 (43) ◽  
pp. 435105 ◽  
Author(s):  
Kaihu Zhang ◽  
Lan Jiang ◽  
Xin Li ◽  
Xuesong Shi ◽  
Dong Yu ◽  
...  

2012 ◽  
Vol 11 (04) ◽  
pp. 709-721 ◽  
Author(s):  
QIAN-ZHEN SU ◽  
JIE YU ◽  
KAI-JUN YUAN ◽  
SHU-LIN CONG

Above-threshold dissociation (ATD) process of the molecular ions HD+ steered by a femtosecond laser pulse train (LPT) is investigated theoretically using the time-dependent quantum wave packet method. Energy-dependent distributions of ATD fragments are analyzed by using an asymptotic-flow expression in the momentum space. It is found that fragment kinetic energy spectra shift to low energy region with increasing pulse number of LPT. The photofragment branching ratio between the 1sσg and 2pσu dissociation channels is sensitive to the pulse number of LPT. The momentum distribution of the ATD fragments is discussed in detail.


2006 ◽  
Author(s):  
Haiyi Sun ◽  
Tianqing Jia ◽  
Xiaoxi Li ◽  
Chengbin Li ◽  
Donghai Feng ◽  
...  

2006 ◽  
Vol 41 (3) ◽  
pp. 447-454 ◽  
Author(s):  
N. Vujičić ◽  
S. Vdović ◽  
D. Aumiler ◽  
T. Ban ◽  
H. Skenderović ◽  
...  

2003 ◽  
Vol 445 (2) ◽  
pp. 182-185 ◽  
Author(s):  
Ken-ichi Kawamura ◽  
Keisuke Maekawa ◽  
Hiroshi Yanagi ◽  
Masahiro Hirano ◽  
Hideo Hosono

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