[1] Zhang J, Wang W M, Yang X H et al. Double-cone ignition scheme for inertial confinement fusion[J]. Philosophical Transactions of the Royal Society A, 378, 20200015(2020).

[2] 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).

[3] Fang K, Zhang Z, Li Y T et al. Analytical studies of Rayleigh-Taylor instability growth of double-cone ignition scheme in 2020 winter experimental campaign[J]. Acta Physica Sinica, 71, 035204(2022).

[4] Zhang Z, Yuan X H, Zhang Y H et al. Efficient energy transition from kinetic to internal energy in supersonic collision of high-density plasma jets from conical implosions[J]. Acta Physica Sinica, 71, 155201(2022).

[5] Zhao X, Yuan X H, Zheng J et al. An angular-resolved scattered-light diagnostic for laser-plasma instability studies[J]. The Review of Scientific Instruments, 93, 053505(2022).

[6] Kruer W L[M]. The physics of laser plasma interactions(1988).

[7] Ji L L, Liu C, Zhu B Q et al. Analysis of influence of beam smoothing on third harmonic generation in SGⅡ upgrade[J]. Acta Optica Sinica, 33, 1219002(2013).

[8] Craxton R S, Anderson K S, Boehly T R et al. Direct-drive inertial confinement fusion: a review[J]. Physics of Plasmas, 22, 110501(2015).

[9] Datte P, Celliers P, Kalantar D et al. Operational experience with optical streak cameras at the National Ignition Facility[J]. Proceedings of SPIE, 8850, 88500G(2013).

[10] Gong T, Zheng J, Li Z C et al. Frequency mismatch in stimulated scattering processes: an important factor for the transverse distribution of scattered light[J]. Physics of Plasmas, 23, 063303(2016).

[11] Bower D E, McCarville T J, Alvarez S S et al. Full aperture backscatter station measurement system on the National Ignition Facility[J]. Review of Scientific Instruments, 75, 4177-4179(2004).

[12] Froula D H, Bower D, Chrisp M et al. Full-aperture backscatter measurements on the national ignition facility[J]. Review of Scientific Instruments, 75, 4168-4170(2004).

[13] Wilke M D, Fernández J C, Berggren R R et al. Full aperture backscatter station imager diagnostics system for far-field imaging of laser plasma instabilities on Nova[J]. Review of Scientific Instruments, 68, 672-675(1997).

[14] Li Z C. Experimental research on large-scale laser-plasma interactions[D](2011).

[15] Wang C K, Jiang X H, Wang Z B et al. Full-aperture backscatter station on Shenguang-Ⅱlaser facility[J]. High Power Laser and Particle Beams, 22, 1896-1900(2010).

[16] Wang F, Peng X S, Yan Y D et al. Backscattered light diagnostic technique based on Shen Guang-Ⅲ laser facility[J]. Chinese Journal of Lasers, 42, 0902011(2015).

[17] Wei H Y, Peng X S, Xu T et al. Full aperture backscatter light diagnostic system on Shenguang-Ⅲ prototype laser facility[J]. High Power Laser and Particle Beams, 24, 2773-2777(2012).

[18] Li Z C, Zhang X D, Yang D et al. Energy fraction measurements of stimulated Brillouin scattering and stimulated Raman scattering on Shenguang-Ⅲ prototype laser facility[J]. High Power Laser and Particle Beams, 22, 1891-1895(2010).

[19] Jiao C Y, Wang F, Jiang X H et al. Full aperture backscatter diagnosis system on Shenguang prototype laser facility[J]. Nuclear Electronics & Detection Technology, 31, 306-311(2011).

[20] Xu S Y, Zhou S L, Gong Y F et al. Influence of continuous phase plate on backscattered transmission characteristics of SBS laser light at target[J]. Acta Optica Sinica, 40, 2205001(2020).

[21] Qiao Z F, Lu X Q, Zhao D F et al. Arrangement design of the final optics assembly for the SG-Ⅱ upgrading laser[J]. Chinese Journal of Lasers, 35, 1328-1332(2008).

[22] Zha W Y, Yang D, Xu T et al. Backscatter spectra measurements of the two beams on the same cone on Shenguang-III laser facility[J]. The Review of Scientific Instruments, 89, 013501(2018).