Programmably repetition tunable low pedestal femtosecond pulse train generation using comb-like profiled fiber

Author(s):  
K. Igarashi ◽  
H. Tobioka ◽  
A. Oguri ◽  
T. Akutsu ◽  
S. Namiki ◽  
...  
1994 ◽  
Vol 19 (8) ◽  
pp. 539 ◽  
Author(s):  
S. V. Chernikov ◽  
R. Kashyap ◽  
J. R. Taylor

2000 ◽  
Vol 12 (2) ◽  
pp. 214-214 ◽  
Author(s):  
K. Vlachos ◽  
T. Houbavlis ◽  
K. Zoiros ◽  
H. Avramopoulos

2016 ◽  
Vol 119 (24) ◽  
pp. 243301 ◽  
Author(s):  
Li-Xiang Hu ◽  
Tong-Pu Yu ◽  
Fu-Qiu Shao ◽  
Wen Luo ◽  
Yan Yin

Laser Physics ◽  
2013 ◽  
Vol 24 (1) ◽  
pp. 016002 ◽  
Author(s):  
Yin Huang ◽  
Ting Xie ◽  
Jian Li ◽  
Jie Yu ◽  
Shu-Lin Cong

2021 ◽  
Vol 255 ◽  
pp. 13004
Author(s):  
Martin Luttmann ◽  
David Bresteau ◽  
Thierry Ruchon

In a recent work [1], we demonstrated how laser-dressed ionization can be harnessed to control with attosecond accuracy the time delay between an extreme-ultraviolet (XUV) attosecond pulse train and an infrared (IR) femtosecond pulse. In this case, the comb-like photoelectron spectrum obtained by ionizing a gas target with the two superimposed beams exhibits peaks oscillating with the delay. Two of them can be found to oscillate in phase quadrature, allowing an optimal measurement and stabilization of the delay over a large range. Here we expand this technique to isolated attosecond pulses, by taking advantage of the delay-modulation of attosecond streaking traces. Although the photoelectron spectrum contains no peaks in that case, it is possible to reconstruct the pump-probe delay by simply monitoring the mean energy of the spectrum and the amplitude at this energy. In general, we find that active delay stabilization based on laser-dressed ionization is possible as long as the XUV pulses are chirped.


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