100 J-level pulse compression for peak power enhancement

Mironov, S. Yu.; Wheeler, Jonathan; Gonin, René; Cojocaru, G.; Ungureanu, R.; Banici, Romeo; Şerbănescu, Mihai; Dabu, R.; Mourou, G.; Хазанов, Е. А.

doi:10.1070/qel16307

Cited by 26 publications

(13 citation statements)

References 7 publications

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“…this work [ 34 ] 2017 [ 35 ] 2018 [ 36 ] 2019 [ 37 ] 2020 [ 38 ] 2020 [ 26 ] 2010 [ 27 ] 2014 [ 28 ] 2016 [ 29 ] 2017 [ 30 ] 2019 [ 31 ] 2019 [ 32 ] 2019 [ 33 ] 2021 [ 34 ] 2017 [ 35 ] 2018 [ 36 ] 2019 [ 37 ] 2020 [ 38 ] 2020 [ 26 ] 2010 [ 27 ] 2014 [ 28 ] 2016 [ 29 ] 2017 [ 30 ] 2019 [ 31 ] 2019 [ 32 ] 2019 [ 33 ] 2021 Fig. 3.…”

Section: Compressed Pulse Duration Fs B-integralmentioning

confidence: 94%

“…this work [ 34 ] 2017 [ 35 ] 2018 [ 36 ] 2019 [ 37 ] 2020 [ 38 ] 2020 [ 26 ] 2010 [ 27 ] 2014 [ 28 ] 2016 [ 29 ] 2017 [ 30 ] 2019 [ 31 ] 2019 [ 32 ] 2019…”

Section: Compressed Pulse Duration Fsmentioning

confidence: 94%

“…Pulse compression factor F τ =τ in /τ out (a) and compressed pulse duration τ out (b) vs B-integral. The colored symbols correspond to the experiments with an input pulse power of 100 TW and more [33][34][35][36][37], all the rest -less than 50 TW [25][26][27][28][29][30][31][32]. The curves in Fig.…”

Section: Compressed Pulse Duration Fs B-integralmentioning

confidence: 99%

“…For example, the application of the method for a pulse after wide-angle non-collinear optical parametric chirped-pulse amplification (WNOPCPA) [19], the enhancement of the pulse time contrast simultaneously with its compression [20][21][22][23], and the use of a nonlinear medium with a large n 2 [24]. Pulse compression of the lasers of moderately low power (below 50 TW) [25][26][27][28][29][30][31][32], as well as of the lasers with a power of 100 TW and higher [33][34][35][36][37] was experimentally demonstrated at free beam propagation in a nonlinear medium. Note also the demonstration of the two-stage CafCA in both these ranges [32,38].…”

Section: Introductionmentioning

confidence: 99%

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11 fs, 1.5 PW Laser with Nonlinear Pulse Compression

Гинзбург

Yakovlev

Kochetkov

et al. 2021

Laser Congress 2021 (ASSL,LAC)

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The PEARL laser output pulse with a duration of 60-70 fs was compressed to 11 fs after passing through a 5-mm thick silica plate and reflecting from two chirping mirrors with a total dispersion of -250 fs 2 . The experiments were carried out for the B-integral values up to 19 without damage of the optical elements, which indicates that small-scale self-focusing was suppressed. The results obtained show the possibility of further nonlinear compression scaling to multipetawatt power in pulses with duration commensurate with the field period.

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Section: Compressed Pulse Duration Fs B-integralmentioning

confidence: 94%

“…this work [ 34 ] 2017 [ 35 ] 2018 [ 36 ] 2019 [ 37 ] 2020 [ 38 ] 2020 [ 26 ] 2010 [ 27 ] 2014 [ 28 ] 2016 [ 29 ] 2017 [ 30 ] 2019 [ 31 ] 2019 [ 32 ] 2019…”

Section: Compressed Pulse Duration Fsmentioning

confidence: 94%

Section: Compressed Pulse Duration Fs B-integralmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

See 2 more Smart Citations

11 fs, 1.5 PW Laser with Nonlinear Pulse Compression

Гинзбург

Yakovlev

Kochetkov

et al. 2021

Laser Congress 2021 (ASSL,LAC)

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“…Subsequent dispersion management (DM) through technology such as negative dispersion chirped mirrors then re-compresses the pulse to the desired shortened duration. This compression technique has been studied at the TW scale [11,12] demonstrating up to five-fold pulse compression [13] and work is now implementing the method on PWscale laser systems [14] . The low energy losses permit the option to employ multiple stages to decrease the pulse to the desired duration [15] .…”

Section: Introductionmentioning

confidence: 99%

Spectral broadening for multi-Joule pulse compression in the APOLLON Long Focal Area facility

Bleotu

Wheeler

Papadopoulos

et al. 2022

High Pow Laser Sci Eng

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Spectral-broadening of the Apollon PW-class laser pulses using a Thin Film Compression technique within the Long-Focal-Area interaction chamber of the APOLLON laser facility is reported, demonstrating the delivery of the full energy pulse to the target interaction area. The laser pulse at 7 J passing through large aperture, thin glass wafers is spectrally broadened to a bandwidth that is compatible with a 15 fs pulse, indicating also the possibility to achieve sub-10 fs pulses using 14 J. Placing the post-compressor near the interaction makes for an economical method to produce the shortest pulses by limiting the need for high damage, broadband optics close to the final target rather than throughout the entire laser transport system.

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