[1] [1] S E Bodner, D G Colombant, J H Gardner, et al.. Direct-drive laser fusion: Status and prospects[J]. Physics of Plasmas, 1998, 5(5): 1901-1918.

[2] [2] S E Bodner, D G Colombant, A J Schmitt, et al.. High-gain direct-drive target design for laser fusion[J]. Physics of Plasmas, 2000, 7(6): 2298-2301.

[3] [3] D G Colombant, S E Bodner, A J Schmitt, et al.. Effects of radiation on direct-drive laser fusion targets[J]. Physics of Plasmas, 2000, 7(5): 2046-2054.

[4] [4] A J Schmitt, D G Colombant, A L Velikovich, et al.. Large-scale high-resolution simulations of high gain direct-drive inertial confinement fusion targets[J]. Physics of Plasmas, 2004, 11(5): 2716-2722.

[5] [5] B Canaud, F Garaude. Optimization of laser-target coupling efficiency for direct drive laser fusion[J]. Nuclear Fusion, 2005, 45(12): L43-L47.

[6] [6] B Canaud, F Garaude, P Ballereau, et al.. High-gain direct-drive inertial confinement fusion for the laser mégajoule: recent progress [J]. Plasma physics and controlled fusion, 2007, 49(12): B601-B610.

[7] [7] D G Colombant, A J Schmitt, S P Obenschain, et al.. Direct-drive laser target designs for sub-megajoule energies[J]. Physics of Plasmas, 2007, 14(5): 56317.

[8] [8] A J Schmitt, J W Bates, S P Obenschain, et al.. Direct drive fusion energy shock ignition designs for sub- MJ lasers[J]. Fusion Science and Technology, 2008, 56(1): 371-383.

[9] [9] M Temporal, B Canaud, B J L Garrec. Irradiation uniformity and zooming performances for a capsule directly driven by a 32M9 laser beams configuration[J]. Physics of Plasmas, 2010, 17(2): 22701.

[10] [10] B Canaud, M Temporal. High-gain shock ignition of direct-drive ICF targets for the laser mégajoule[J]. New Journal of Physics, 2010, 12(04): 43037.

[11] [11] J W Bates, A J Schmitt, D E Fyfe, et al.. Simulations of high-gain shock-ignited inertial-confinement-fusion implosions using less than 1 MJ of direct KrF laser energy[J]. High Energy Density Physics, 2010, 6(2): 128-134.

[12] [12] J D Sethian, M Friedman, E Al. Electron beam pumped KrF lasers for fusion energy[J]. Physics of Plasmas, 2003, 10(5): 2142-2146.

[13] [13] S P Obenschain, J D Sethian, A J Schmit. A laser based fusion test facility[J]. Fusion Science and Technology, 2009, 56(2): 594-603.

[14] [14] S P Obenschain, C J Pawley, K Gerber, et al.. Uniform target accelaration and imprinting studies with the nike KrF lasers[C]. Conference on Lasers and Electro-Optics, 1997: CThJ2.

[15] [15] J D Sethian, S P Obenschain, K A Gerber, et al.. Large area electron beam pumped krypton fluoride laser amplifier[J]. Review of Scientific Instruments, 1997, 68(6): 2357-2366.

[16] [16] S P Obenschain, D G Colombant, A J Schmitt, et al.. Pathway to a lower cost high repetition rate ignition facility[J]. Physics of Plasmas, 2006, 13(5): 36320.

[17] [17] J L Weaver, S P Obenschain, J D Sethian, et al.. Advantages of KrF lasers for inertial confinement fusion energy[C]. 23rd IAEA Fusion Energy Conference, 2010: 6-7.

[18] [18] J D Sethian, D G Colombant, J L Giuliani, et al.. The science and technologies for fusion energy with lasers and direct drive targets [J]. IEEE Transactions on Plasma Science, 2010, 38(4): 690-703.

[19] [19] R Lehmberg, J Goldhar. Use of incoherence to produce smooth and controllable irradiation profiles with KrF fusion lasers[J]. Fusion Technology, 1987, 11(3): 532-541.

[20] [20] D M Kehne, M Karasik, Y Aglitsky, et al.. Implementation of focal zooming on the Nike KrF laser[J]. Review of Scientific Instruments, 2013, 84: 013509.

[21] [21] Hu Yun, Zhao Xueqing, Xue Quanxi, et al.. ASE Suppression in the high power excimer laser MOPA system based on electrooptical switch[J]. Chinese J Lasers, 2013, 40(1):0102008.

[22] [22] Hu Yun, Zhao Xueqing, Xue Quanxi, et al.. High contrast ratio ultraviolet electro-optical switch[J]. High Power Laser and Particle Beams, 2013, 25(3): 561-564.

[23] [23] Hu Yun, Zhao Xueqing, Xue Quanxi, et al.. Suppression of ASE from excimer laser using cascaded UV electro-optical switch[J]. Optics and Precission Engineering, 2013, 21(1): 13-19.