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

[2] Zheng W G, Wei X F, Zhu Q H et al. SG-III laser facility has successfully achieved 60 TW/180 kJ ultraviolet laser (351 nm) output[J]. High Power Laser and Particle Beams, 28, 091901(2016).

[3] Pérez F, Kay J J, Patterson J R et al. Efficient laser-induced 6-8 keV X-ray production from iron oxide aerogel and foil-lined cavity targets[J]. Physics of Plasmas, 19, 083101(2012). http://scitation.aip.org/content/aip/journal/pop/19/8/10.1063/1.4740076

[4] Brown C G, Bond E. Clancy T, et al. Assessment and mitigation of electromagnetic pulse (EMP) impacts at short-pulse laser facilities[J]. Journal of Physics: Conference Series, 244, 032001(2010). http://adsabs.harvard.edu/abs/2010JPhCS.244c2001B

[5] Dubois J L, Lubrano-Lavaderci F, Raffestin D et al. Target charging in short-pulse-laser-plasma experiments[J]. Physical Review E, 89, 013102(2014). http://europepmc.org/abstract/med/24580341

[6] Lion C. The LMJ program: an overview[J]. Journal of Physics: Conference Series, 244, 012003(2010). http://adsabs.harvard.edu/abs/2010JPhCS.244a2003L

[7] Fournier K B, Satcher J H, May M J et al. Absolute X-ray yields from laser-irradiated germanium-doped low-density aerogels[J]. Physics of Plasmas, 16, 052703(2009). http://scitation.aip.org/content/aip/journal/pop/16/5/10.1063/1.3140041

[8] Jacquet L, Girard F, Primout M et al. Multi-keV X-ray sources from metal-lined cylindrical hohlraums[J]. Physics of Plasmas, 19, 083301(2012). http://scitation.aip.org/content/aip/journal/pop/19/8/10.1063/1.4746031

[9] de Marco M, Pfeifer M, Krousky E et al. . Basic features of electromagnetic pulse generated in a laser-target chamber at 3-TW laser facility PALS[J]. Journal of Physics: Conference Series, 508, 012007(2014). http://adsabs.harvard.edu/abs/2014JPhCS.508a2007D

[10] Fournier K B, May M J, Colvin J D et al. Demonstration of a 13-keV KrK-shell X-ray source at the National Ignition Facility[J]. Physical Review E, 88, 033104(2013). http://europepmc.org/abstract/med/24125368

[11] May M J, Fournier K B, Colvin J D et al. Bright X-ray stainless steel K-shell source development at the National Ignition Facility[J]. Physics of Plasmas, 22, 063305(2015). http://scitation.aip.org/content/aip/journal/pop/22/6/10.1063/1.4922751

[12] Meng C, Yang C, Li X et al. Development of electromagnetic environment research of high power laser facility[J]. Journal of Terahertz Science and Electronic Information Technology, 15, 70-74(2017).

[13] Jin H B, Meng C, Jiang Y S et al. Simulation of electromagnetic pulses generated by escaped electrons in a high-power laser chamber[J]. Plasma Science and Technology, 20, 115201(2018). http://www.cnki.com.cn/Article/CJFDTotal-DNZK201811006.htm

[14] Meng C, Xu Z Q, Jiang Y S et al. Numerical simulation of the SGEMP inside a target chamber of a laser inertial confinement facility[J]. IEEE Transactions on Nuclear Science, 64, 2618-2625(2017). http://ieeexplore.ieee.org/document/8012488/

[15] Meng C, Xu Z Q. Numerical simulation of EMP environment radiated by X-rays inside a high-power laser facility. [C]∥2018 International Applied Computational Electromagnetics Society Symposium in Denver, March 25-29, 2018. Denver, Co, USA. New York: IEEE, 17803175(2018).

[16] Beers B L. Radiation-induced signals in cables-II[J]. IEEE Transactions on Nuclear Science, 24, 2429-2434(1977). http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=4328602

[17] Xu Z Q, Meng C. Evaluation of cable SGEMP response using Monte Carlo and finite-difference time-domain methods[J]. IEEE Transactions on Nuclear Science, 64, 2829-2836(2017). http://adsabs.harvard.edu/abs/2017ITNS...64.2829X

[18] Li J X, Cheng Y H, Zhou H et al. Calculation of coaxial line X-ray responses by transmission line method and finite difference time domain method[J]. High Power Laser and Particle Beams, 19, 2079-2082(2007).