[1] Ditmire T, Bless S, Dyer G, et al. Overview of future directions in high energy-density and high-field science using ultra-intense lasers[J]. Radiation Physics and Chemistry, 70, 535-552(2004).
[2] Ravasio A, Gregori G, Benuzzi-Mounaix A, et al. Direct observation of strong ion coupling in laser-driven shock-compressed targets[J]. Physical Review Letters, 99, 135006(2007).
[3] Barbrel B, Koenig M, Benuzzi-Mounaix A, et al. Measurement of short-range correlations in shock-compressed plastic by short-pulse X-ray scattering[J]. Physical Review Letters, 102, 165004(2009).
[4] Lee H J, Neumayer P, Castor J, et al. X-ray Thomson-scattering measurements of density and temperature in shock-compressed beryllium[J]. Physical Review Letters, 102, 115001(2009).
[5] Lee H J, Workman J, Wark J S, et al. Optically induced lattice dynamics probed with ultrafast X-ray diffraction[J]. Physical Review B, 77, 132301(2008).
[6] Kalantar D H, Belak J F, Collins G W, et al. Direct observation of the
[8] Malone R M, Capelle G A, Celeste J R, et al. Overview of the lineimaging VISAR diagnostic at the National Ignition Facility (NIF)[C]Proceedings of SPIE 6342, International Optical Design Conference 2006. Vancouver, 2006: 634220.
[9] Celliers P M, Bradley D K, Collins G W, et al. Line-imaging velocimeter for shock diagnostics at the OMEGA laser facility[J]. Review of Scientific Instruments, 75, 4916-4929(2004).
[10] Trott W M, Renlund A M, Jungst R G. Singlepulse Raman photoacoustic spectroscopy studies of triaminotrinitrobenzene (TATB) related compounds[C]Proceedings of SPIE 0540, Southwest Conf on Optics ''85. Albuquerque, 1985: 368375.
[11] Asay J R, Hall C A, Konrad C H, et al. Use of Z-pinch sources for high-pressure equation-of-state studies[J]. International Journal of Impact Engineering, 23, 27-38(1999).
[12] Chhabildas L C, Trott W M, Reinhart W D, et al. Incipient spall studies in tantalum-microstructural effects[J]. AIP Conference Proceedings, 620, 483-486(2002).
[14] Reich C, Gibbon P, Uschmann I, et al. Yield optimization and time structure of femtosecond laser plasma Kα sources[J]. Physical Review Letters, 84, 4846-4849(2000).
[15] Wang Hongjian, Ye Yan, Li Jun, et al. Doublespectrum imaging device driven by laser to generate Xray source: 201210252295.2[P]. 20121114
[17] Singh T, Kahlon K S, Dhaliwal A S. Total bremsstrahlung spectral photon distributions in metallic targets in the photon energy range of 5–10 keV by 204Tl beta particles[J]. Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, 267, 737-741(2009).
[18] Wang Hongjian, Li Zeren, Chen Zhanbin. High conversion efficiency and small spot size of Kα X-ray generated from nano-foam Cu targets irradiated by femtosecond laser pulses[J]. Applied Physics B, 124, 172(2018).
[19] Xiong Yong. Conversion efficiencies of ultrasht ultraintensity laser to ultra hot based on Ka X ray electron[D]. Beijing: China Academy of Engineering Physics, 2008: 9092
[21] Liu Hongjie, Gu Yuqiu, Zhou Weimin, et al. Characterization of relativistic electrons generated by a cone guiding laser pulse[J]. Chinese Physics B, 21, 055207(2012).
[23] Liu Yanli. Study on industrial Xray image sharpening technology algithm[D]. Taiyuan: Nth University of China, 2015
[24] Li Chenguang. Synthetical NDT image processing f weld joint of pipeline[D]. Qingdao: China University of Petroleum (East China), 2011).
[26] Mao J Y, Chen L M, Ge X L, et al. Spectrally peaked electron beams produced via surface guiding and acceleration in femtosecond laser-solid interactions[J]. Physical Review E, 85, 025401(2012).
