• High Power Laser and Particle Beams
  • Vol. 32, Issue 1, 011008 (2020)
Ping Li, Jun Zhang, and Xiaofeng Wei
Author Affiliations
  • Research Center of Laser Fusion, CAEP, P. O. Box 919-988, Mianyang 621900, China
  • show less
    DOI: 10.11884/hplpb202032.190466 Cite this Article
    Ping Li, Jun Zhang, Xiaofeng Wei. Plasma optics technologies: State of the art and future perspective[J]. High Power Laser and Particle Beams, 2020, 32(1): 011008 Copy Citation Text show less
    Temperature and density range of typical plasma
    Fig. 1. Temperature and density range of typical plasma
    Area division of distribution of permittivity and permeablity of materials
    Fig. 2. Area division of distribution of permittivity and permeablity of materials
    Schematic diagram of PEPC
    Fig. 3. Schematic diagram of PEPC
    Schematic diagram of low loss PEPC based on DKDP crystal
    Fig. 4. Schematic diagram of low loss PEPC based on DKDP crystal
    Design diagram of reflective PEPC
    Fig. 5. Design diagram of reflective PEPC
    Basic principle of laser amplification based on plasma medium
    Fig. 6. Basic principle of laser amplification based on plasma medium
    (a) The gas-filled balloon target is used to create a uniform plasma to amplify a single seed beam (red) by combination of eight pumping beams (yellow), (b) the incident power of all the beams
    Fig. 7. (a) The gas-filled balloon target is used to create a uniform plasma to amplify a single seed beam (red) by combination of eight pumping beams (yellow), (b) the incident power of all the beams
    Laser pulse-shape conditioning with a double plasma-mirror (DPM)
    Fig. 8. Laser pulse-shape conditioning with a double plasma-mirror (DPM)
    Temporal profile of the laser pulses delivered by a 10 TW, 60 fs laser system, in logarithmic scale, with and without DPM
    Fig. 9. Temporal profile of the laser pulses delivered by a 10 TW, 60 fs laser system, in logarithmic scale, with and without DPM
    (a) Experimental setup for tight focusing of ultrahigh-intensity laser pulses by low F-number confocal EPM. (b) Focal spot provided by the conventional F/2.7 output. (c) Focal spot in the output of the F/0.4, images are in common logarithm scale
    Fig. 10. (a) Experimental setup for tight focusing of ultrahigh-intensity laser pulses by low F-number confocal EPM. (b) Focal spot provided by the conventional F/2.7 output. (c) Focal spot in the output of the F/0.4, images are in common logarithm scale
    (a) Schematic diagram of cross beam interaction in plasma. (b) Excitation characteristics of cross beam energy transfer and phase shift
    Fig. 11. (a) Schematic diagram of cross beam interaction in plasma. (b) Excitation characteristics of cross beam energy transfer and phase shift
    Conceptual design of plasma polarizer and plasma wave plate
    Fig. 12. Conceptual design of plasma polarizer and plasma wave plate
    The extreme Faraday effect of strongly magnetized plasma
    Fig. 13. The extreme Faraday effect of strongly magnetized plasma
    Schematic of the target arrangement to study the interaction of the PII-beam with a solid target
    Fig. 14. Schematic of the target arrangement to study the interaction of the PII-beam with a solid target
    Schematic of a plasma optical modulator
    Fig. 15. Schematic of a plasma optical modulator
    Schematic diagram of plasma holographic formation process
    Fig. 16. Schematic diagram of plasma holographic formation process
    Characteristics of Q-plate based on magnetized plasma
    Fig. 17. Characteristics of Q-plate based on magnetized plasma
    Ping Li, Jun Zhang, Xiaofeng Wei. Plasma optics technologies: State of the art and future perspective[J]. High Power Laser and Particle Beams, 2020, 32(1): 011008
    Download Citation