2021
DOI: 10.1364/oe.424356
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Multistep pulse compressor for 10s to 100s PW lasers

Abstract: High-energy tens (10s) to hundreds (100s) petawatt (PW) lasers are key tools for exploring frontier fundamental researches such as strong-field quantum electrodynamics (QED), and the generation of positron-electron pair from vacuum. Recently, pulse compressor became the main obstacle on achieving higher peak power due to the limitation of damage threshold and size of diffraction gratings. Here, we propose a feasible multistep pulse compressor (MPC) to increase the maximum bearable input and output pulse energi… Show more

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Cited by 22 publications
(33 citation statements)
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“…Another possible solution is to use two matched gratings or deformable gratings as the second and the third gratings in the main compressor to compensate each other; [ 360 ] or to introduce a wavefront‐correction plate or a deformable mirror in the main compressor (between the second and the third gratings) to correct the overlaid wavefront of the second and the third gratings. [ 284,361 ] In our opinion, this complex spatiotemporal distortion in technology is not a fatal problem for the next‐generation short‐pulse PW laser, although it now becomes more and more serious in current short‐pulse PW lasers, especially in high average‐power TW/PW lasers.…”
Section: Bottlenecksmentioning
confidence: 99%
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“…Another possible solution is to use two matched gratings or deformable gratings as the second and the third gratings in the main compressor to compensate each other; [ 360 ] or to introduce a wavefront‐correction plate or a deformable mirror in the main compressor (between the second and the third gratings) to correct the overlaid wavefront of the second and the third gratings. [ 284,361 ] In our opinion, this complex spatiotemporal distortion in technology is not a fatal problem for the next‐generation short‐pulse PW laser, although it now becomes more and more serious in current short‐pulse PW lasers, especially in high average‐power TW/PW lasers.…”
Section: Bottlenecksmentioning
confidence: 99%
“…That is why kinds of technologies for beam smoothing and spatial noise (spatial frequency) filtering have been widely used in almost all nanosecond, picosecond, and femtosecond high-energy lasers. [279][280][281][282][283][284][285][286] Even in air/vacuum, Figure 19f,g shows a simulation result: after 2 m long free propagation, diffraction also degrades both the intensity and wavefront profiles and leads to energy lost. Here, based on a 300 nm (700-1000 nm) broadband intense laser pulsed beam, the simulation shows that SSSF has limited spectral dependence due to a short interaction length in media (see Figure 19d,e), while long-distance free propagation in air/vacuum introduces obvious spatiospectral coupling (accordingly spatiotemporal coupling) in both amplitude (intensity) and phase (wavefront) (see Figure 19f,g).…”
Section: Beam Qualitymentioning
confidence: 99%
“…These problems can be solved in the whole system design in Ref. [15] by a reflective deformable mirror (DM). Actually, the induced spatial dispersion width is small in comparison to the beam size, and the transmitted light owning small wavefront distortion.…”
Section: Discussionmentioning
confidence: 99%
“…Recently, it was reported that this spatiotemporal focusing can be used in ultrahighpeak-power laser systems with large beam sizes [20][21][22][23]. In this MPC optical design, the intentionally induced spatial dispersion using a grating or prism pair was used to smoothen the laser beam with large beam sizes to reduce its LSIMR [15].…”
Section: Principle Of Prism-pair-induced Spatial and Spectral Dispers...mentioning
confidence: 99%
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