High power all-fiber picosecond laser system for UV light generation

2012 ◽  
Author(s):  
M. Oku ◽  
K. Kieu ◽  
N. Peyghambarian
Keyword(s):  
High Power ◽  
Uv Light ◽  
Laser System ◽  
Picosecond Laser ◽  
Light Generation

Optimal design of a high-power picosecond laser system using a dual-stage ytterbium-doped fibre amplifier

Laser Physics ◽  
2013 ◽  
Vol 23 (7) ◽  
pp. 075114 ◽  
Author(s):  
Yi-Jing You ◽  
Chih-Hsuan Lin ◽  
Alexey Zaytsev ◽  
Feng-Hua Tsai ◽  
Chi-Luen Wang ◽  
...  
Keyword(s):  
Optimal Design ◽  
High Power ◽  
Laser System ◽  
Picosecond Laser ◽  
Fibre Amplifier ◽  
Dual Stage

High-power picosecond laser system with a slab neodymium glass amplifier operating at a repetition frequency up to 1 Hz

1986 ◽  
Vol 16 (12) ◽  
pp. 1582-1585 ◽  
Author(s):  
A Varanavichyus ◽  
R Grigonis ◽  
R Danelyus ◽  
A Piskarskas ◽  
D Podenas
Keyword(s):  
High Power ◽  
Laser System ◽  
Picosecond Laser ◽  
Repetition Frequency ◽  
Neodymium Glass

scholarly journals Compact 50 W All-Solid-State Picosecond Laser System at 1 kHz

2020 ◽  
Vol 10 (19) ◽  
pp. 6891
Author(s):  
Shuaishuai Yang ◽  
Zijian Cui ◽  
Ziming Sun ◽  
Pan Zhang ◽  
Dean Liu
Keyword(s):  
Laser Pulse ◽  
High Power ◽  
Thermal Lens ◽  
Traveling Wave ◽  
Repetition Rate ◽  
Laser System ◽  
Picosecond Laser ◽  
Regenerative Amplifier ◽  
Lens Effect ◽  
Thermal Lens Effect

Compact, stable, high-power and high repetition rate picosecond laser systems are excellent sources for optical parametric chirped pulse amplification systems and laser satellite ranging systems. Compared with the traditional complex high-power amplifier, this article reports a compact high-power picosecond laser system at a repetition rate of 1 kHz based on Nd:YAG bulk crystal. The thermal lens effect limits the regenerative amplifier to directly output higher energy. For this reason, multi-stage traveling-wave amplifiers are usually used to gradually increase the laser pulse energy. So as to achieve a compact structure, a regenerative amplifier that can output higher power at 1 kHz is designed in the laser system. The regenerative amplifier can output the power of 6.5 W at the pump power of 41.5 W; the beam quality of M2 factor was about 1.3. A more flexible thermal depolarization compensation structure is applied in the side-pumped amplifier, which can effectively compensate for thermal lens effect and thermal depolarization at different pump powers. Finally, the laser pulse can achieve an output power higher than 50 W at 1 kHz after passing through an end-pumped traveling-wave amplifier and a side-pumped traveling wave amplifier.

High power 808 nm VCSEL arrays for pumping of compact pulsed high energy Nd:YAG lasers operating at 946 nm and 1064 nm for blue and UV light generation

2011 ◽  
Author(s):  
Robert Van Leeuwen ◽  
Yihan Xiong ◽  
Laurence S. Watkins ◽  
Jean-Francois Seurin ◽  
Guoyang Xu ◽  
...  
Keyword(s):  
High Power ◽  
Uv Light ◽  
High Energy ◽  
Nd:Yag Lasers ◽  
Light Generation ◽  
Vcsel Arrays

High power picosecond laser system at 248 nm

1988 ◽  
Vol 59 (10) ◽  
pp. 2235-2240 ◽  
Author(s):  
W. Tighe ◽  
C. H. Nam ◽  
J. Robinson ◽  
S. Suckewer
Keyword(s):  
High Power ◽  
Laser System ◽  
Picosecond Laser

Compact high power Raman laser system using phase-modulated sidebands amplified by a single tapered amplifier

CPEM 2010 ◽  
2010 ◽  
Author(s):  
K. S. Lee ◽  
S. E. Park ◽  
T. Y. Kwon ◽  
S. B. Lee ◽  
J. Kim
Keyword(s):  
High Power ◽  
Laser System ◽  
Raman Laser

ALD anti-reflection coatings at 1ω, 2ω, 3ω, and 4ω for high-power ns-laser application

2018 ◽  
Vol 7 (1-2) ◽  
pp. 23-31 ◽  
Author(s):  
Hao Liu ◽  
Lars Jensen ◽  
Ping Ma ◽  
Detlev Ristau
Keyword(s):  
High Power ◽  
High Surface ◽  
Laser System ◽  
Damage Threshold ◽  
Atomic Layer ◽  
Intensity Difference ◽  
High Power Laser ◽  
Power Laser ◽  
Laser Applications ◽  
Laser Induced Damage

AbstractAtomic layer deposition (ALD) facilitates the deposition of coatings with precise thickness, high surface conformity, structural uniformity, and nodular-free structure, which are properties desired in high-power laser coatings. ALD was studied to produce uniform and stable Al2O3and HfO2single layers and was employed to produce anti-reflection coatings for the harmonics (1ω, 2ω, 3ω, and 4ω) of the Nd:YAG laser. In order to qualify the ALD films for high-power laser applications, the band gap energy, absorption, and element content of single layers were characterized. The damage tests of anti-reflection coatings were carried out with a laser system operated at 1ω, 2ω, 3ω, and 4ω, respectively. The damage mechanism was discussed by analyzing the damage morphology and electric field intensity difference. ALD coatings exhibit stable growth rates, low absorption, and rather high laser-induced damage threshold (LIDT). The LIDT is limited by HfO2as the employed high-index material. These properties indicate the high versatility of ALD films for applications in high-power coatings.

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