A mathematical model of the removal of gold thin film on polymer surface by laser ablation

2005 ◽  
Vol 190 (2-3) ◽  
pp. 260-263 ◽  
Author(s):  
X.L. Zhou ◽  
W. Wen ◽  
J.S. Zhang ◽  
D.B. Sun
2014 ◽  
Vol 550 ◽  
pp. 190-198 ◽  
Author(s):  
S. Amoruso ◽  
N.N. Nedyalkov ◽  
X. Wang ◽  
G. Ausanio ◽  
R. Bruzzese ◽  
...  

2011 ◽  
Vol 110 (12) ◽  
pp. 124303 ◽  
Author(s):  
S. Amoruso ◽  
N. N. Nedyalkov ◽  
X. Wang ◽  
G. Ausanio ◽  
R. Bruzzese ◽  
...  

Author(s):  
M. Grant Norton ◽  
C. Barry Carter

Pulsed-laser ablation has been widely used to produce high-quality thin films of YBa2Cu3O7-δ on a range of substrate materials. The nonequilibrium nature of the process allows congruent deposition of oxides with complex stoichiometrics. In the high power density regime produced by the UV excimer lasers the ablated species includes a mixture of neutral atoms, molecules and ions. All these species play an important role in thin-film deposition. However, changes in the deposition parameters have been shown to affect the microstructure of thin YBa2Cu3O7-δ films. The formation of metastable configurations is possible because at the low substrate temperatures used, only shortrange rearrangement on the substrate surface can occur. The parameters associated directly with the laser ablation process, those determining the nature of the process, e g. thermal or nonthermal volatilization, have been classified as ‘primary parameters'. Other parameters may also affect the microstructure of the thin film. In this paper, the effects of these ‘secondary parameters' on the microstructure of YBa2Cu3O7-δ films will be discussed. Examples of 'secondary parameters' include the substrate temperature and the oxygen partial pressure during deposition.


Author(s):  
Jin Young Kim ◽  
R. E. Hummel ◽  
R. T. DeHoff

Gold thin film metallizations in microelectronic circuits have a distinct advantage over those consisting of aluminum because they are less susceptible to electromigration. When electromigration is no longer the principal failure mechanism, other failure mechanisms caused by d.c. stressing might become important. In gold thin-film metallizations, grain boundary grooving is the principal failure mechanism.Previous studies have shown that grain boundary grooving in gold films can be prevented by an indium underlay between the substrate and gold. The beneficial effect of the In/Au composite film is mainly due to roughening of the surface of the gold films, redistribution of indium on the gold films and formation of In2O3 on the free surface and along the grain boundaries of the gold films during air annealing.


Author(s):  
Babak Soltani ◽  
Faramarz Hojati ◽  
Amir Daneshi ◽  
Bahman Azarhoushang

AbstractUnderstanding the laser ablation mechanism is highly essential to find the effect of different laser parameters on the quality of the laser ablation. A mathematical model was developed in the current investigation to calculate the material removal rate and ablation depth. Laser cuts were created on the workpiece with different laser scan speeds from 1 to 10 mm s−1 by an ultrashort pulse laser with a wavelength of about 1000 nm. The calculated depths of laser cuts were validated via practical experiments. The variation of the laser power intensity on the workpiece’s surface during laser radiation was also calculated. The mathematical model has determined the laser-material interaction mechanism for different laser intensities. The practical sublimation temperature and ablated material temperature during laser processing are other data that the model calculates. The results show that in laser power intensities (IL) higher than 1.5 × 109 W cm−2, the laser-material interaction is multiphoton ionisation with no effects of thermal reaction, while in lower values of IL, there are effects of thermal damages and HAZ adjacent to the laser cut. The angle of incidence is an essential factor in altering incident IL on the surface of the workpiece during laser processing, which changes with increasing depth of the laser cut.


2021 ◽  
Vol 1098 (6) ◽  
pp. 062062
Author(s):  
R Fahdiran ◽  
I Sugihartono ◽  
E Handoko ◽  
E Budi ◽  
A B Susila ◽  
...  

1998 ◽  
Vol 66 (2) ◽  
pp. 183-187 ◽  
Author(s):  
M. Diegel ◽  
F. Falk ◽  
R. Hergt ◽  
H. Hobert ◽  
H. Stafast

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