Broadband second harmonic generation of spatially chirped pulses

Yudong Tao; Dongxia Hu; Wei Han

doi:10.11884/HPLPB202032.190146

[1] Ed G. Laser physics: extreme light[J]. Nature, 446, 8-16(2007).

[2] Danson C, Hillier D, Hopps N. Petawatt class lasers worldwide[J]. High Power Laser Science and Engineering, 5-18(2015).

[5] Néauport J, Journot E, Gaborit G. Design, optical characterization, and operation of large transmission gratings for the laser integration line and laser megajoule facilities[J]. Applied Optics, 44, 3143-3152(2005).

[7] Mero M, Petrov V. High-power, few-cycle, angular dispersion compensated mid-infrared pulses from a noncollinear optical parametric amplifier[J]. IEEE Photonics Journal, 9, 1-8(2017).

[8] Richter T, SchtLanghst C, Elschner R, et al. Distributed 1Tbs alloptical aggregation capacity in 125GHz optical bwidth by frequency conversion in fiber[C]IEEE European Conference on Optical Communication (ECOC). 2015.

[9] Dontsova E I, Vatnik I D, Babin S A. Frequency doubling of Raman fiber lasers with random distributed feedback[J]. Optics Letters, 41, 1439-1442(2016).

[10] Lanka N R, Patnaik S A, Harjani R A. Frequency-hopped quadrature frequency synthesizer in 0.13-μm technology[J]. IEEE Journal of Solid-State Circuits, 46, 2021-2032(2011).

[12] Zhu H, Wang T, Zheng W. Efficient second harmonic generation of femtosecond laser at 1 μm[J]. Optics Express, 12, 2150-2155(2004).

[13] Kanai T, Zhou X, Sekikawa T. Generation of subterawatt sub-10-fs blue pulses at 1-5 kHz by broadband frequency doubling[J]. Optics Letters, 28, 1484-1486(2003).

[14] Schmidt B E, Nicolas Thiré, Boivin M. High gain-frequency domain optical parametric amplification (FOPA)[J]. Nature Communications, 5, 3643-3644(2014).

[15] Gruson V, Ernotte G, Lassonde P. 2.5 TW, two-cycle IR laser pulses via frequency domain optical parametric amplification[J]. Optics Express, 25, 27706(2017).