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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- High Power Laser and Particle Beams
- Vol. 34, Issue 1, 011001 (2022)
![Schematic of laser-plasma process in the underdense plasma corona, inverse bremsstrahlung absorption occurs up to critical density[4]](/richHtml/qjglzs/2022/34/1/011001/img_1.jpg)
Fig. 1. Schematic of laser-plasma process in the underdense plasma corona, inverse bremsstrahlung absorption occurs up to critical density[4]

Fig. 2. Laser platforms for creating high-pressure experiments
![Thermodynamic compression paths within the sample for the case of laser-based compression[14]](/Images/icon/loading.gif)
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]](/Images/icon/loading.gif)
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]](/Images/icon/loading.gif)
Fig. 5. Temperature evolution in dynamic compression, ideal isentrope, ideal Hugoniot curve and ramp compression[20]

Fig. 6. Experimental design of material compression based on laser facilities

Fig. 7. Three types of moving reflecting surfaces in the interferometer velometer
![Example of a laser indirect driven shock+ramp compression experiment[37-38]](/Images/icon/loading.gif)

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]](/Images/icon/loading.gif)
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]](/Images/icon/loading.gif)
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]](/Images/icon/loading.gif)
Fig. 12. A high-resolution spectrometer in NIF and spectral data of an undriven Cu sample[63]

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]](/Images/icon/loading.gif)
Fig. 14. Experimental setup and date analysis of laser indirect drive shockless isentropic compression of Au and Pt[1]

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]](/Images/icon/loading.gif)
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]](/Images/icon/loading.gif)
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]

Fig. 18. Continuous measurement of sound velocity along Hugoniot curve via lateral release method

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