• High Power Laser and Particle Beams
  • Vol. 34, Issue 1, 011001 (2022)
Mu Li1, Hongping Zhang2, Shi Chen1, Peidong Tao1、3, Hang Zhu1, Cangtao Zhou1, Jianheng Zhao4, and Chengwei Sun5、6
Author Affiliations
  • 1Shenzhen Key Laboratory of Ultra-intense Laser and Advanced Material Technology, Center for Advanced Material Diagnostic Technology, College of Engineering Physics, Shenzhen Technology University, Shenzhen 518118, China
  • 2Big Data and Internet College, Shenzhen Technology University, Shenzhen 518118, China
  • 3College of Physics, Sichuan University, Chengdu 610065, China
  • 4Institute of Applied Electronics, CAEP, Mianyang 621900, China
  • 5Institute of Fluid Physics, CAEP, Mianyang 621900, China
  • 6Shanghai Institute of Laser Plasma, CAEP, Shanghai 201800, China
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    DOI: 10.11884/HPLPB202234.210357 Cite this Article
    Mu Li, Hongping Zhang, Shi Chen, Peidong Tao, Hang Zhu, Cangtao Zhou, Jianheng Zhao, Chengwei Sun. Laser driven dynamic compression of materials[J]. High Power Laser and Particle Beams, 2022, 34(1): 011001 Copy Citation Text show less
    Schematic of laser-plasma process in the underdense plasma corona, inverse bremsstrahlung absorption occurs up to critical density[4]
    Fig. 1. Schematic of laser-plasma process in the underdense plasma corona, inverse bremsstrahlung absorption occurs up to critical density[4]
    Laser platforms for creating high-pressure experiments
    Fig. 2. Laser platforms for creating high-pressure experiments
    Thermodynamic compression paths within the sample for the case of laser-based compression[14]
    Fig. 3. Thermodynamic compression paths within the sample for the case of laser-based compression[14]
    Ramp quasi-isentropic compression: kinematics illustration, measurements, data analysis[1]
    Fig. 4. Ramp quasi-isentropic compression: kinematics illustration, measurements, data analysis[1]
    Temperature evolution in dynamic compression, ideal isentrope, ideal Hugoniot curve and ramp compression[20]
    Fig. 5. Temperature evolution in dynamic compression, ideal isentrope, ideal Hugoniot curve and ramp compression[20]
    Experimental design of material compression based on laser facilities
    Fig. 6. Experimental design of material compression based on laser facilities
    Three types of moving reflecting surfaces in the interferometer velometer
    Fig. 7. Three types of moving reflecting surfaces in the interferometer velometer
    Example of a laser indirect driven shock+ramp compression experiment[37-38]
    Fig. 8. Example of a laser indirect driven shock+ramp compression experiment[37-38]
    Design of a streaked optical pyrometer system together with VISAR in the laser driven platform
    Fig. 9. Design of a streaked optical pyrometer system together with VISAR in the laser driven platform
    Designed intensity of streaked optical pyrometer (SOP) with brightness temperature (left) and SOP intensity vs shock velocity (right)[55]
    Fig. 10. Designed intensity of streaked optical pyrometer (SOP) with brightness temperature (left) and SOP intensity vs shock velocity (right)[55]
    Spectral radiance measured at the interface of iron/LiF in gas gun platform. (a) raw data of a 16-channel time resolved optical pyrometer; (b) the fitted curve to determine the temperature and emissivity of iron[59]
    Fig. 11. Spectral radiance measured at the interface of iron/LiF in gas gun platform. (a) raw data of a 16-channel time resolved optical pyrometer; (b) the fitted curve to determine the temperature and emissivity of iron[59]
    A high-resolution spectrometer in NIF and spectral data of an undriven Cu sample[63]
    Fig. 12. A high-resolution spectrometer in NIF and spectral data of an undriven Cu sample[63]
    Dynamic X-ray diffraction mode based on laser drive platform
    Fig. 13. Dynamic X-ray diffraction mode based on laser drive platform
    Experimental setup and date analysis of laser indirect drive shockless isentropic compression of Au and Pt[1]
    Fig. 14. Experimental setup and date analysis of laser indirect drive shockless isentropic compression of Au and Pt[1]
    Raw VISAR data from the D2 cryogenic experiment in NIF and measured phase diagram for the D2 insulator to metal transition measured by different experiments
    Fig. 15. Raw VISAR data from the D2 cryogenic experiment in NIF and measured phase diagram for the D2 insulator to metal transition measured by different experiments
    Laser driven shock loading of static pre-compressed H-He mixture, the target structure, raw data of SOP and VISAR, phase diagram of H, He, and the mixture[22]
    Fig. 16. Laser driven shock loading of static pre-compressed H-He mixture, the target structure, raw data of SOP and VISAR, phase diagram of H, He, and the mixture[22]
    (a) Electrical conductivity of water from different experiment, electronic conductivity from laser shocked water ice with static pre-compression, shock reverberation (solid blue) and principal Hugoniot (black) of water[23]; (b) experimental data from Hugoniot of water ice VII and shock reverberation of liquid water, novel superionic water ice was found as fcc structure (red)[69]
    Fig. 17. (a) Electrical conductivity of water from different experiment, electronic conductivity from laser shocked water ice with static pre-compression, shock reverberation (solid blue) and principal Hugoniot (black) of water[23]; (b) experimental data from Hugoniot of water ice VII and shock reverberation of liquid water, novel superionic water ice was found as fcc structure (red)[69]
    Continuous measurement of sound velocity along Hugoniot curve via lateral release method
    Fig. 18. Continuous measurement of sound velocity along Hugoniot curve via lateral release method
    Mu Li, Hongping Zhang, Shi Chen, Peidong Tao, Hang Zhu, Cangtao Zhou, Jianheng Zhao, Chengwei Sun. Laser driven dynamic compression of materials[J]. High Power Laser and Particle Beams, 2022, 34(1): 011001
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