pulse amplification
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2022 ◽  
Vol 148 ◽  
pp. 107791
Author(s):  
Fenxiang Wu ◽  
Xingyan Liu ◽  
Xinliang Wang ◽  
Jiabing Hu ◽  
Xiaoming Lu ◽  
...  

2022 ◽  
Vol 20 (3) ◽  
pp. 031405
Author(s):  
Zexing Zhao ◽  
Hao Chen ◽  
Ziming Zhang ◽  
Jiatong Li ◽  
Fangxiang Zhu ◽  
...  

2021 ◽  
Author(s):  
Ji Wang ◽  
Yanqing Zheng ◽  
Yunlin Chen

Abstract Optical parametric chirped pulse amplification (OPCPA) shows great potential in producing ultrashort high-intensity pulses because of its large gain bandwidth. Quasi-parametric chirped pulse amplification (QPCPA) may further extend the bandwidth, but the behavior of QPCPA at a limited pump intensity (e.g., ≤5 GW/cm2 in a nanosecond pumped QPCPA) is not fully investigated yet. We have discussed in detail the ultra-broadband amplification and the noncollinear phase-matching geometry in QPCPA. We have modeled and developed a novel noncollinear geometry in QPCPA namely ’triple-wavelength phase-matching geometry’ which provides two additional phase-matching points around the phase-matching point at the center wavelength. Our analysis demonstrates that the triple-wavelength phase-matching geometry can support stable, ultra-broadband amplification in QPCPA. The numerical simulation results show that ultrashort pulse with a pulse duration of 7.92 fs can be achieved in QPCPA when the pump intensity is limited to 5 GW/cm2, calculated using the nonlinear coefficient of YCOB.


2021 ◽  
Author(s):  
Chengyong Feng ◽  
Christophe Dorrer ◽  
Cheonha Jeon ◽  
Rick Roides ◽  
Benjamin Webb ◽  
...  

Photonics ◽  
2021 ◽  
Vol 8 (11) ◽  
pp. 471
Author(s):  
Aleksei Abramov ◽  
Igor Zolotovskii ◽  
Vladimir Kamynin ◽  
Victor Prikhodko ◽  
Aleksei Tregubov ◽  
...  

We explored the dynamics of frequency-modulated (FM) pulses in a cascaded fiber configuration comprising one active and one passive optical fiber with multiple fiber Bragg gratings (FBGs) of different periods inscribed over the fiber configuration length. We present a theoretical formalism to describe the mechanisms of the FM pulse amplification and pulse compression in such fiber cascades resulting in peak powers up to ~0.7 MW. In combination with the decreasing dispersion fibers, the considered cascade configuration enables pico- and sub-picosecond pulse trains with a sub-terahertz repetition rate and sub-kW peak power generated directly from the continuous optical signal.


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