[1] Danson C N, Haefner C, Bromage J et al. Petawatt and exawatt class lasers worldwide[J]. High Power Laser Science and Engineering, 7, e54(2019).

[2] Danson C, Hillier D, Hopps N et al. Petawatt class lasers worldwide[J]. High Power Laser Science and Engineering, 3, e3(2015).

[3] Esarey E, Schroeder C B, Leemans W P. Physics of laser-driven plasma-based electron accelerators[J]. Reviews of Modern Physics, 81, 1229-1285(2009).

[4] Macchi A, Borghesi M, Passoni M. Ion acceleration by superintense laser-plasma interaction[J]. Reviews of Modern Physics, 85, 751-793(2013).

[5] Roth M, Jung D, Falk K et al. Bright laser-driven neutron source based on the relativistic transparency of solids[J]. Physical Review Letters, 110, 044802(2013).

[6] Lindl J. Development of the indirect-drive approach to inertial confinement fusion and the target physics basis for ignition and gain[J]. Physics of Plasmas, 2, 3933-4024(1995).

[7] Lindl J D, Amendt P, Berger R L et al. The physics basis for ignition using indirect-drive targets on the National Ignition Facility[J]. Physics of Plasmas, 11, 339-491(2004).

[8] Stephens R B, Hatchett S P, Turner R E et al. Implosion of indirectly driven reentrant-cone shell target[J]. Physical Review Letters, 91, 185001(2003).

[9] Park H S, Chambers D M, Chung H K et al. High-energy Kα radiography using high-intensity, short-pulse lasers[J]. Physics of Plasmas, 13, 056309(2006).

[10] Miller G H, Moses E I, Wuest C R. The National Ignition Facility: enabling fusion ignition for the 21st century[J]. Nuclear Fusion, 44, S228-S238(2004).

[11] Tommasini R, MacPhee A, Hey D et al. 79(10): 10E901(2008).

[12] Stuart B C, Bonlie J D, Britten J A et al. The Titan laser at LLNL. [C]∥2006 Conference on Lasers and Electro-Optics and 2006 Quantum Electronics and Laser Science Conference, May 21-26, 2006, Long Beach, CA, USA. New York: IEEE, 4628707(2006).

[13] Kelly J H, Waxer L J, Bagnoud V et al. OMEGA EP: high-energy petawatt capability for the OMEGA laser facility[J]. Journal de Physique IV, 133, 75-80(2006).

[14] Barty C, Key M, Britten J et al. An overview of LLNL high-energy short-pulse technology for advanced radiography of laser fusion experiments[J]. Nuclear Fusion, 44, S266-S275(2004).

[15] Zhu J Q, Chen S H, Zheng Y X et al. Review on development of Shenguang-Ⅱ laser facility[J]. Chinese Journal of Lasers, 46, 0100002(2019).

[16] Zhu J Q, Zhu J, Li X C et al. Status and development of high-power laser facilities at the NLHPLP[J]. High Power Laser Science and Engineering, 6, e55(2018).

[17] Chen H, Hermann M R, Kalantar D H et al. High-energy (>70 keV) X-ray conversion efficiency measurement on the ARC laser at the National Ignition Facility[J]. Physics of Plasmas, 24, 033112(2017).

[18] Zhu Q H, Zhou K N, Su J Q et al. The Xingguang-III laser facility: precise synchronization with femtosecond, picosecond and nanosecond beams[J]. Laser Physics Letters, 15, 015301(2018).

[19] Tommasini R, Hatchett S P, Hey D S et al. Development of Compton radiography of inertial confinement fusion implosions[J]. Physics of Plasmas, 18, 056309(2011).

[20] Tommasini R, Bailey C, Bradley D K et al. Short pulse, high resolution, backlighters for point projection high-energy radiography at the National Ignition Facility[J]. Physics of Plasmas, 24, 053104(2017).

[21] Tian C, Yu M H, Shan L Q et al. Radiography of direct drive double shell targets with hard X-rays generated by a short pulse laser[J]. Nuclear Fusion, 59, 046012(2019).