Chinese Journal of Lasers, Volume. 51, Issue 11, 1101005(2024)
Research Progress, Technical Challenges, and Development Trends in High‑Energy Picosecond Petawatt Lasers
Fig. 1. SG-II-UP picosecond petawatt laser. (a) Left beamline of SG-II-UP is picosecond petawatt laser; (b) schematic diagram of a picosecond petawatt laser; (c) large-aperture pulse compression grating
Fig. 3. Improvement of SNR for laser seed source in SG-II-UP PW. (a) Schematic of ps-OPA[62]; (b) measurement results of SNR enhancement
Fig. 4. Pre-pulses and stray light sources of a multi-pass amplifier. (a) Schematic of a multi-pass amplifier; (b) two types of pencil beam
Fig. 5. SNR measurement results of a multi-pass amplifier. (a) Pre-pulses in time range when PEPC is on; (b) pre-pulses outside time range when PEPC is on
Fig. 6. Main wave aberrations affecting focusing ability of a picosecond petawatt laser
Fig. 10. Focusing ability of SG-II-UP PW laser. (a) Residual wavefront error: PV of 0.57λ, RMS of 0.11λ; (b) focal spot measured by X-ray pinhole camera [FWHM 17.0 μm(H)×20.8 μm(V)]; (c) measurement results of far-field focal spot; (d) encircled energy analysis of focal spot distribution in (c)
Fig. 11. High fidelity focal spot measurement technology[118-123]. (a)(b) Indirect measurement technology of focal spot and algorithm in OMEGA-EP based on phase recovery algorithm; (c) an in-situ focal-spot microscope used in OMEGA-EP; (d) diagram of indirect measurement technology of focal spot based on coherent modulation imaging in SG-II-UP PW; (e)(f) comparison of indirect and direct measurements of focal spot in SG-II-UP PW
Fig. 12. Laser pulse distribution with different STCs[108]. (a) Laser pulse with PFT; (b) laser pulse with PFC; (c)(d) spatial phase distribution for three different frequencies ω1 <ω0 <ω2 of pulse for (a) and (b), respectively
Fig. 14. Application of an focused plasma mirror based on ellipsoid[131]. (a) Experimental diagram; (b) focal spot distribution in traditional off-axis parabolic mirror focusing system; (c) distribution of focal spot under ellipsoidal focusing plasma mirror
Fig. 15. Output capability analysis of SG-II-UP PW. (a)(b) Output capability of a multi-pass amplifier; (c) near field distribution of main amplifier; (d) near field distribution after pulse compression
Fig. 16. Online damage measurement technology for large-aperture grating. (a) Schematic of dark-field scattering imaging; (b) damage measurement result of a grating G4
Fig. 17. Technology of active laser-pointing stabilization[146]. (a) Schematic of active laser-pointing stabilization control system in SG-II-UP PW system; (b) measurement result of the laser pointing stability in open-loop and in closed-loop
Fig. 18. Schematic overview of hundred terawatt undulator (HTU) experimental setup with active control system of laser pointing[148]
Fig. 19. Schematic of optomechanical coupling active control for spatial filter system of a PW laser[149]
Fig. 21. Synchronization measurement of LMJ-PETAL[160]. (a) Schematic diagram of 2D-SI; (b)(c) images of fringes for a delay of 50 fs and for a delay of 3 ps respectively
Fig. 23. Pulse amplification and compression technology in a plasma. (a) Joule level sc-SBS plasma amplification results[180];
|
Get Citation
Copy Citation Text
Youen Jiang, Pengqian Yang, Xue Pan, Yanli Zhang, Yajing Guo, Ping Zhu, Dawei Li, Yong Cui, Ouyang Xiaoping, Hua Tao, Zhuocai Jiang, Quantang Fan, Neng Hua, Shunxing Tang, Qi Xiao, Dongjun Zhang, Dongning Liu, Pengfei Huang, Zuqiang Li, Baoqiang Zhu, Weixin Ma. Research Progress, Technical Challenges, and Development Trends in High‑Energy Picosecond Petawatt Lasers[J]. Chinese Journal of Lasers, 2024, 51(11): 1101005
Category: laser devices and laser physics
Received: Feb. 15, 2024
Accepted: Apr. 22, 2024
Published Online: Jun. 6, 2024
The Author Email: Jiang Youen (joyen@siom.ac.cn), Yang Pengqian (jqzhu@siom.ac.cn)
CSTR:32183.14.CJL240591