High Power Laser Science and Engineering, Volume. 8, Issue 4, 04000e31(2020)
Ultra-broadband all-OPCPA petawatt facility fully based on LBO Editors' Pick
Fig. 2. Simulated spectra at each stage of the system with LBO and the front end with BBO.
Fig. 3. Simulated spectra at each stage of the system compared with the expected efficiency of the compressor.
Fig. 4. Measured spectrum of the Ti:sapphire system showing intensity modulation.
Fig. 5. Sketch of the picosecond mJ-level front end experimental setup. The commercial Ti:sapphire oscillator (Venteon) and the two commercial RGAs (S-pulse and Magma25) are seeding and pumping the four NOPA stages, respectively. The compact seed stretcher is made by two BK7 glass blocks, as shown below the Venteon box. The violet dashed boxes are hybrid achromatic telescopes (ACTs, described in
Fig. 6. Spatial profile of (top) the S-pulse output on the SHG crystal and (bottom) the SHG pump.
Fig. 7. (Top) BBO efficiency (
Fig. 8. Spatial profile of (top) the Magma25 output on the SHG crystal and (bottom) the SHG pump.
Fig. 10. Near-field spatial profile of the output of (top) the first and (bottom) the second amplification stages.
Fig. 11. Stability measurements performed on the NOPA2 pulses power reveal that the system is autonomously stable for about 22 min with RMS values of 3.7%. The NOPA1 PD signal value is increased by a factor of 0.3V to be better represented in the figure.
Fig. 13. Near-field spatial profile of the output of (top) the third and (bottom) the fourth amplification stages.
Fig. 14. Stability measurements performed on the NOPA4 pulses power reveal that the system is autonomously stable for about 1 h with an RMS value of around 4%. After 1 h, a drift is noticeable and the RMS value is degraded to 10%.
Fig. 15. Single-grating compressor stage sketch. Note: CM, corner mirror; M, mirror; GR, grating (line density = 1000 lines/mm,
Fig. 16. Profiles of compressed pulses measured with SPIDER diagnostics: (a) compressed NOPA4 temporal profile; (b), (c) stability measurement performed on the temporal length of the compressed NOPA4 output reveals that the system is autonomously stable for almost 60 min.
Fig. 17. Sketch of the nanosecond J-level front end experimental setup. The commercial Nd:YAG laser is pumping the three NOPA stages. The violet dashed boxes are hybrid ACTs (described in
Fig. 18. Design of a Nd:glass chain for the first high-energy pump. A 100 mW CW laser is sliced with a fiber EOM and successively amplified in a fiber to reach the nJ level. This is then amplified in an RGA to 1 mJ and injected into the chain. Note: F1, F2, Faraday; 9AMP, 16AMP, 25AMP, 45AMP, amplifiers with respective diameters in mm; SF, spatial filter; L, lens; PH, pinhole; VSF1, VSF2, vacuum spatial filters; RWP, rotating wave-plate to control output energy; λ/2, half-wave plate.
Fig. 20. Telescope between the ns OPCPA and the first high-energy OPCPA stage: (a) sketch in the OpticStudio environment; (b) residual optical path.
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Mario Galletti, Pedro Oliveira, Marco Galimberti, Munadi Ahmad, Giedre Archipovaite, Nicola Booth, Emerald Dilworth, Andy Frackiewicz, Trevor Winstone, Ian Musgrave, Cristina Hernandez-Gomez. Ultra-broadband all-OPCPA petawatt facility fully based on LBO[J]. High Power Laser Science and Engineering, 2020, 8(4): 04000e31
Category: Research Articles
Received: Jun. 9, 2020
Accepted: Aug. 4, 2020
Published Online: Oct. 9, 2020
The Author Email: Mario Galletti (mario.galletti@lnf.infn.it)