High energy 40 fs compact diode-pumped femtosecond laser for nanostructuring applications

2006 ◽  
Author(s):  
Clemens Hönninger ◽  
Ramatou Bello Doua ◽  
Eric P. Mottay ◽  
François Salin
Keyword(s):  
Femtosecond Laser ◽  
High Energy ◽  
Diode Pumped

POLARIS - A High Energy, 2.5x10^11 Temporal Contrast, High Intensity Diode Pumped Solid State Laser

2014 ◽  
Author(s):  
Marco Hornung ◽  
Sebastian Keppler ◽  
Alexander Kessler ◽  
Hartmut Liebetrau ◽  
Andreas Seidel ◽  
...  
Keyword(s):  
Solid State ◽  
High Intensity ◽  
High Energy ◽  
Solid State Laser ◽  
Temporal Contrast ◽  
State Laser ◽  
Diode Pumped

High energy diode pumped 5th harmonic generation of Nd: YAG laser

2013 ◽  
Author(s):  
Yang Yu ◽  
Chee Yuen Cheng ◽  
Yong Poo Chia ◽  
Wee Hoong Wong ◽  
Saw Soon Yong ◽  
...  
Keyword(s):  
Harmonic Generation ◽  
High Energy ◽  
Yag Laser ◽  
Diode Pumped

scholarly journals High-energy, diode-pumped, nanosecond Yb:YAG MOPA system

2008 ◽  
Vol 16 (6) ◽  
pp. 3674 ◽  
Author(s):  
M. Siebold ◽  
J. Hein ◽  
C. Wandt ◽  
S. Klingebiel ◽  
F. Krausz ◽  
...  
Keyword(s):  
High Energy ◽  
Diode Pumped

Demonstration of a diode pumped Nd,Y co-doped SrF 2 crystal based, high energy chirped pulse amplification laser system

2017 ◽  
Vol 382 ◽  
pp. 201-204 ◽  
Author(s):  
Junchi Chen ◽  
Yujie Peng ◽  
Zongxin Zhang ◽  
Hongpeng Su ◽  
Yuxin Leng ◽  
...  
Keyword(s):  
Laser System ◽  
High Energy ◽  
Chirped Pulse ◽  
Pulse Amplification ◽  
Chirped Pulse Amplification ◽  
Diode Pumped ◽  
Co Doped

Wavelength tunable, high energy femtosecond laser pulses directly generated from large-mode-area photonic crystal fiber

2012 ◽  
Vol 285 (10-11) ◽  
pp. 2715-2718 ◽  
Author(s):  
Chi Zhang ◽  
Yu-ying Zhang ◽  
Ming-lie Hu ◽  
Si-jia Wang ◽  
You-jian Song ◽  
...  
Keyword(s):  
Photonic Crystal ◽  
Femtosecond Laser ◽  
Photonic Crystal Fiber ◽  
Laser Pulses ◽  
High Energy ◽  
Femtosecond Laser Pulses ◽  
Large Mode Area ◽  
Crystal Fiber ◽  
Wavelength Tunable ◽  
Mode Area

scholarly journals HELL: High-Energy Electrons by Laser Light, a User-Oriented Experimental Platform at ELI Beamlines

2018 ◽  
Vol 8 (9) ◽  
pp. 1565 ◽  
Author(s):  
Tadzio Levato ◽  
Stefano Bonora ◽  
Gabriele Grittani ◽  
Carlo Lazzarini ◽  
Muhammad Nawaz ◽  
...  
Keyword(s):  
Laser Light ◽  
Accelerate Electron ◽  
Electron Acceleration ◽  
High Energy ◽  
Experimental Platform ◽  
Secondary Sources ◽  
Wake Field ◽  
High Energy Electrons ◽  
New Ideas ◽  
Diode Pumped

Laser wake field acceleration (LWFA) is an efficient method to accelerate electron beams to high energy. This is a benefit in research infrastructures where a multidisciplinary environment can benefit from the different secondary sources enabled, having the opportunity to extend the range of applications that is accessible and to develop new ideas for fundamental studies. The ELI Beamline project is oriented to deliver such beams to the scientific community both for applied and fundamental research. The driver laser is a Ti:Sa diode-pumped system , running at a maximum performance of 10 Hz, 30 J, and 30 fs. The possibilities to setup experiments using different focal lengths parabolas, as well as the possibility to counter-propagate a second laser beam intrinsically synchronized, are considered in the electron acceleration program. Here, we review the laser-driven electron acceleration experimental platform under implementation at ELI Beamlines, the HELL (High-energy Electrons by Laser Light) experimental platform .

scholarly journals Space-Selective Control of Functional Crystals by Femtosecond Laser: A Comparison between SrO-TiO2-SiO2 and Li2O-Nb2O5-SiO2 Glasses

Crystals ◽  
2020 ◽  
Vol 10 (11) ◽  
pp. 979
Author(s):  
Xuan He ◽  
Qiming Liu ◽  
Matthieu Lancry ◽  
François Brisset ◽  
Bertrand Poumellec
Keyword(s):  
Femtosecond Laser ◽  
Second Harmonic ◽  
Scanning Speed ◽  
High Energy ◽  
Femtosecond Laser Irradiation ◽  
Laser Polarization ◽  
Electron Backscattered Diffraction ◽  
Sio2 Glass ◽  
Significant Difference ◽  
Induced Crystallization

We report on space-selective crystallization of congruent and polar Sr2TiSi2O8 crystals in a stoichiometric SrO-TiO2-SiO2 glass induced by (1030 nm, 300 fs) femtosecond laser irradiation. This allows us to compare with non-congruent laser-induced crystallization of polar LiNbO3 in non-stoichiometric Li2O-Nb2O5-SiO2 glass and gain information on the mechanism of nanocrystals orientation with the laser polarization that we pointed out previously. Using scanning electron microscopy (SEM), second harmonic generation (SHG), and electron backscattered diffraction (EBSD), we studied the laser-induced crystallization according to the laser processing parameters (pulse energy, pulse repetition rate, scanning speed). We found (1) a domain where the laser track is filled with crystals not perfectly textured (low energy), (2) a domain where an amorphous volume remains surrounded by a crystallized shell (high energy). This arises from Sr out-diffusion and may give rise to the crystallization of both SrTiO3 and Sr2TiSi2O8 phases at low speed. In the one-phase domain (at higher speed), the possibility to elaborate a tube with a perfect Fresnoite texture is found. A significant difference in size and morphology whereas the crystallization threshold remains similar is discussed based on glass thermal properties. Contrarily to Li2O-Nb2O5-SiO2 (LNS) glass, no domain of oriented nanocrystallization controlled by the laser polarization has been found in SrO-TiO2-SiO2 (STS) glass, which is attributed to the larger crystallization speed in STS glass. No nanogratings have also been found that is likely due to the congruency of the glass.

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