Burst mode PCS of EPON

2005 ◽  
Author(s):  
Xiao Du
Keyword(s):  
2014 ◽  
Vol E97.B (2) ◽  
pp. 432-440 ◽  
Author(s):  
Masamichi FUJIWARA ◽  
Ken-Ichi SUZUKI ◽  
Naoto YOSHIMOTO
Keyword(s):  

2020 ◽  
Vol 38 (6) ◽  
pp. 1330-1340 ◽  
Author(s):  
Alex Forencich ◽  
Valerija Kamchevska ◽  
Nicolas Dupuis ◽  
Benjamin G. Lee ◽  
Christian W. Baks ◽  
...  

2014 ◽  
Vol 39 (2) ◽  
pp. 236 ◽  
Author(s):  
P. Elahi ◽  
S. Yılmaz ◽  
Y. B. Eldeniz ◽  
F. Ö. Ilday

Laser Physics ◽  
2016 ◽  
Vol 26 (2) ◽  
pp. 025104 ◽  
Author(s):  
Kaihua Wei ◽  
Pinghui Wu ◽  
Ruhua Wen ◽  
Jiangxin Song ◽  
Yan Guo ◽  
...  
Keyword(s):  

2020 ◽  
Vol 127 (1) ◽  
Author(s):  
Daniel Metzner ◽  
Peter Lickschat ◽  
Steffen Weißmantel

AbstractThe authors report on the results of surface treatment experiments using a solid-state amplified laser source emitting laser pulses with a pulse duration of 10 ps. The laser source allows the generation of pulse trains (bursts) with an intra-burst pulse repetition rate of 80 MHz (pulse-to-pulse time interval about 12.5 ns) with up to eight pulses per burst. In this study a wavelength of 1064 nm was used to investigate both ablation of material and laser-induced surface modifications occuring in metallic implant alloys CoCrMo (cobalt-chromium-molybdenum) and TiAlV (titanium-aluminum-vanadium) in dependence of the number of pulses and fluences per pulse in the burst. By using the burst mode, a smoothing effect occurs in a certain parameter range, resulting in very low surface roughness of the generated microstructures. It is demonstrated that at fluences per pulse which are smaller than the material-specific ablation threshold, a self-organized pore formation takes place if a defined number of pulses per burst is used. Thus, the advantage of the MHz burst mode in terms of a possible surface modification is established.


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