Design of comb-like profiled fiber for efficient pulse compression based on stationary rescaled-pulse propagation

Author(s):  
T. Inoue ◽  
H. Tobioka ◽  
K. Igarashi ◽  
S. Namiki
2001 ◽  
Vol 6 (2) ◽  
pp. 51-69 ◽  
Author(s):  
A. Kurtinaitis ◽  
A. Dementjev ◽  
F. Ivanauskas

We describe the simulations of the second harmonic generation of ultrashort laser pulses by numerically solving a system of wave propagation equations. The equations are solved by using a split-step method in twodimensional cyllindrically symmetric space and time coordinates. The diffraction part of a solution uses the Hopscotch type finite-difference scheme on a regular grid. The transport part is solved by using the cubic spline approximation. The obtained numerical results satisfactorily respect energy conservation constraints. The algorithm and program developed make it possible to optimize the process of the second harmonics generation and to identify the conditions where sufficiently high degree of the pulse compression with a relatively low degradation of their quality is achieved.


2003 ◽  
Vol 12 (03) ◽  
pp. 291-305 ◽  
Author(s):  
M. N. VINOJ ◽  
A. U. SEEMA ◽  
V. C. KURIAKOSE

We propose soliton pulse compression mechanism in a dispersion decreasing fiber for the integrable case. We have studied the pulse propagation through various dispersion-decreasing profiles in the adiabatic approximation limit. Out of the different profiles studied, Gaussian profile is found to be the best choice for achieving maximum pulse compression and is found that compressed pulse is completely free from pedestals.


2003 ◽  
Vol 39 (5) ◽  
pp. 401-404 ◽  
Author(s):  
Jianping Wang ◽  
Yue Wu ◽  
Caiyun Lou ◽  
Yizhi Gao

1998 ◽  
Vol 59 (1) ◽  
pp. 91-96 ◽  
Author(s):  
S. SHIBU ◽  
JETENDRA PARASHAR ◽  
H. D. PANDEY

On account of nonlinear refraction, arising through the relativistic mass effect, a short intense laser pulse tends to accumulate its energy around the intensity maximum, leading to pulse compression over a length Zc≈ τ0c2ω2/ ω2pv, where τ0 and ω are the pulse duration and frequency of the laser, v is the oscillatory electron velocity and ωp is the plasma frequency. When the transverse extent of the laser is finite, nonlinear self-focusing interferes strongly with this process. The self-focusing occurs in a periodic manner on a shorter scale length. However, over long lengths of pulse propagation, pulse compression could be significant.


2007 ◽  
Vol 32 (18) ◽  
pp. 2695 ◽  
Author(s):  
Takashi Inoue ◽  
Yuki Taniguchi ◽  
Jiro Hiroishi ◽  
Takeshi Yagi ◽  
Yu Mimura

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Shunsuke Inoue ◽  
Shuji Sakabe ◽  
Yoshihide Nakamiya ◽  
Masaki Hashida

AbstractWe report the generation of ultrashort bright electron pulses directly driven by irradiating a solid target with intense femtosecond laser pulses. The duration of electron pulses after compression by a phase rotator composed of permanent magnets was measured as 89 fs via the ponderomotive scattering of electron and laser pulses, which were almost at the compression limit due to the dispersion of the electron optics. The electron pulse compression system consisting of permanent magnets enabled extremely high timing stability between the laser pulse and electron pulse. The long-term RMS arrival time drift was below 14 fs in 4 h, which was limited by the resolution of the current setup. Because there was no time-varying field to generate jitter, the timing jitter was essentially reduced to zero. To demonstrate the capability of the ultrafast electron pulses, we used them to directly visualize laser pulse propagation in a vacuum and perform 2D mapping of the electric fields generated by low-density plasma in real time.


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