[1] Maiman T H. Stimulated optical radiation in ruby [J].Nature, 1960, 187(4736): 493-494.
[2] Song H H, Wang W M, Li Y T. Dense polarized positrons from laser-irradiated foil targets in the QED regime [J].Phys Rev Lett., 2022, 129(3): 0350011-0350016.
[3] Kodama R, Norreys P A, MimaK, et al. Fast heating of ultrahigh density plasma as a step towards laser fusion ignition [J]. Nature, 2001, 412(6849): 798-802.
[4] Faure J, Rechatin C, Norlin A, et al. Letters controlled injection and acceleration of electrons in plasma wakefields by colliding laser pulses [J]. Nature, 2006,444(7120): 737-739.
[5] Schwoerer H, Pfotenhauer S, Jckel O, et al. Laser-plasma acceleration of quasi-monoenergetic protons from microstructured targets [J]. Nature, 2006, 439(7075):445.
[6] Zhang Z L, Chen Y P, Cui S, et al. Manipulation of polarizations for broadband terahertz waves emitted from laser plasma filaments [J]. Nature Photonics, 2018, 12(9):554-559.
[7] Gregori G, Ravasio A, Murphy C D, et al. Generation of scaled protogalactic seed magnetic fields in laser-produced shock waves [J]. Nature, 2012, 481(7382):480-483.
[8] Luo J, Chen M, Wu W Y, et al. Multistage coupling of laser-wakefield accelerators with curved plasma channels[J]. Phys Rev Lett., 2018, 120(15): 1548011-1548016.
[9] Olshevsky V, Lapenta G, Markidis S. Energetics of kinetic reconnection in a three-dimensional null-point cluster [J]. Phys Rev Lett., 2013, 111(4): 45002.
[10] Birdsall C K, Langdon A B. Plasma physics via computer simulation [M]. New York: Adam Hilger, 1991.
[11] Tajima T, Lee Y C. Absorbing boundary condition and Budden turning point technique for electromagnetic plasma simulations [J]. Journal of Computational Physics,1981, 42(2): 406-412.
[12] Umeda T, Omura Y, Tominaga T, et al. A new charge conservation method in electromagnetic particle-in-cell simulations [J]. Computer Physics Communications,2003, 156(1): 73-85.
[13] Silvester P P, Ferrari R L. Finite elements for electrical engineers [M]. Cambridge Univ. Press, 1983: 113-144.
[14] Loos D. The general particle tracer (GPT) code [J].Gerontechnology, 2006, 20(3-4): 21-30.
[15] 邵福球. 等离子体粒子模拟 [M]. 北京: 科学出版社,2002: 36-108.
[16] Wu Hui-Chun. JPIC & how to make a PIC code [J].Physics, 2011, arXiv: 1104.3163.
[17] Pfund R, Lichters R, Meyer-Ter-Vehn J. LPIC++ a parallel one-dimensional relativistic electromagnetic particle-in-cell code for simulating laser-plasma-interaction [J]. American Institute of Physics, 1998,426(1): 141-146.
[18] Villasenor J, Buneman O. Rigorous charge conservation for local electromagnetic field solvers [J]. Computer Physics Communications, 1992, 69(2-3): 306-316.
[19] Esirkepov T Z. Exact charge conservation scheme for particle-in-cell simulation with an arbitrary form-factor[J]. Computer Physics Communications, 2001, 135(2):144-153.
[20] 陈民. 超短超强激光脉冲与等离子体相互作用中高能粒子发射和加速的理论模拟研究 [D]. 北京: 中国科学院物理研究所, 2007.
[21] Wang W M, Gibbon P, Sheng Z M, et al. Integrated simulation approach for laser-driven fast ignition [J].Phys. Rev. E, 2015, 91(1): 013101.
[22] Wang W M, Gibbon P, Sheng Z M, et al. Laser opacity in under dense preplasma of solid targets due to quantum electrodynamics effects [J]. Phys. Rev. E, 2017, 96(1-1):013201.
[23] Kruer W L. The physics of laser plasma interactions [M].USA: Westview Press, 2001.
[24] Tajima T, Dawson J M. Laser electron accelerator [J].Phys Rev Lett., 1979, 43(4): 267-270.
[25] 盛政明. 强场激光物理研究前沿 [M]. 上海: 上海交通大学出版社, 2014. 323-462.
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