scholarly journals A 33.2 W High Beam Quality Chirped-Pulse Amplification-Based Femtosecond Laser for Industrial Processing

Materials ◽  
2020 ◽  
Vol 13 (12) ◽  
pp. 2841
Author(s):  
Zhenao Bai ◽  
Zhenxu Bai ◽  
Xiaolong Sun ◽  
Yong Liang ◽  
Kun Wang ◽  
...  

A photonic crystal fiber-based chirped pulse amplification delivering 272 fs pulses of 66.4 µJ energy at a repetition rate of 500 kHz is presented, resulting in an average/peak power of 33.2 W/244 MW. A single grating is adopted for the pulse width stretching and compression, which leads to high-compactness and low cost of the system. The output beam is near-diffraction-limited (M2 = 1.1 ± 0.05) with a power stability better than 0.5%. The cutting of alumina ceramic substrate and flexible printed circuit are demonstrated by using the laser system. The results indicate that the laser is competent for industrial applications.

1999 ◽  
Vol 17 (2) ◽  
pp. 341-347
Author(s):  
C.N. DANSON ◽  
R. ALLOTT ◽  
G. BOOTH ◽  
J. COLLIER ◽  
C.B. EDWARDS ◽  
...  

The technique of Chirped Pulse Amplification (CPA) developed by Strickland and Mourou (1985) is now in common use on many laser systems [see, for instance, the review by Perry & Mourou (1994)] and has resulted in massive increases in focused intensities. This paper describes CPA implementation on the Vulcan laser system which has generated multi-Joule sub-picosecond pulses whilst maintaining beam quality to produce focused intensities of 5 × 1019 Wcm−2.


2017 ◽  
Vol 382 ◽  
pp. 201-204 ◽  
Author(s):  
Junchi Chen ◽  
Yujie Peng ◽  
Zongxin Zhang ◽  
Hongpeng Su ◽  
Yuxin Leng ◽  
...  

2020 ◽  
Vol 8 ◽  
Author(s):  
Huijun He ◽  
Jun Yu ◽  
Wentao Zhu ◽  
Xiaoyang Guo ◽  
Cangtao Zhou ◽  
...  

Abstract This study develops a Yb:KGW dual-crystal based regenerative amplifier. The thermal lensing and gain-narrowing effects are compensated by the dual-crystal configuration. Sub-nanojoule pulses are amplified to 1.5 mJ with 9 nm spectral bandwidth and 1 kHz repetition rate using chirped pulse amplification technology. Consequently, 1.2 mJ pulses with a pulse duration of 227 fs are obtained after compression. Thanks to the cavity design, the output laser was a near diffraction limited beam with M2 around 1.1. The amplifier has the potential to boost energy above 2 mJ after compression and act as a front end for a future kilohertz terawatt-class diode-pumped Yb:KGW laser system.


2007 ◽  
Vol 4 (6) ◽  
pp. 421-427 ◽  
Author(s):  
V V Lozhkarev ◽  
G I Freidman ◽  
V N Ginzburg ◽  
E V Katin ◽  
E A Khazanov ◽  
...  

2016 ◽  
Vol 41 (13) ◽  
pp. 3006 ◽  
Author(s):  
Hartmut Liebetrau ◽  
Marco Hornung ◽  
Sebastian Keppler ◽  
Marco Hellwing ◽  
Alexander Kessler ◽  
...  

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