DUAL-BEAM ABLATION OF FUSED QUARTZ USING 266 NM AND VUV LASERS WITH DIFFERENT DELAY-TIMES

Citation
J. Zhang et al., DUAL-BEAM ABLATION OF FUSED QUARTZ USING 266 NM AND VUV LASERS WITH DIFFERENT DELAY-TIMES, Applied physics A: Materials science & processing, 64(5), 1997, pp. 477-481
Citations number
9
Categorie Soggetti
Physics, Applied
ISSN journal
09478396
Volume
64
Issue
5
Year of publication
1997
Pages
477 - 481
Database
ISI
SICI code
0947-8396(1997)64:5<477:DAOFQU>2.0.ZU;2-F
Abstract
The dual-beam laser ablation of fused quartz by 266 nm laser coupled w ith vacuum-ultraviolet (VUV) laser beams at various delay-times of 30 ps, 2 ns, 4 ns, 8 ns and 1 s between VUV and 266 nm beams is reported. The dual-beam ablation method greatly reduced debris deposition at th e circumference and increased the ablation rate in comparison with sin gle-beam ablation. The delay-time effect on the ablation reflects the roles of excited-state and stationary absorption to 266 nm laser. The high-quality ablation can be realized at the delay-times within 4 ns d ue to large excited-state absorption. The surface roughness values at the circumference of patterned structure are 46.2 for 30 ps, 48.2 for 2 ns, and 55.0 nm for 4 ns, respectively. The ablation quality deterio rates with a large surface roughness of 79.3 nm when delay-time increa ses to 8 ns. When delay-time reaches to 1 s, the ablation quality gets even worse with a larger surface roughness of 119.0 nm, but is better than when only 266 nm laser is used due to the stationary effect. In addition, the surface roughness for 266 nm laser is increased to 176.0 nm. In the meanwhile, the ablation rate of 37 and 22 nm/pulse at 30 p s and 8 ns, respectively, indicates an influence of delay-time on the ablation rate. The ablation mechanism is discussed on the basis of the excited-state and stationary absorption to 266 nm laser.