神光Ⅱ装置上间接驱动烧蚀瑞利-泰勒不稳定性实验分析
吴俊峰, 缪文勇, 王立锋, 曹柱荣, 郁晓瑾, 叶文华, 郑无敌, 刘杰, 王敏, 江少恩, 裴文兵, 朱少平, 丁永坤, 张维岩, 贺贤土. 神光Ⅱ装置上间接驱动烧蚀瑞利-泰勒不稳定性实验分析[J]. 强激光与粒子束, 2015, 27(3): 032009.
Wu Junfeng, Miao Wenyong, Wang Lifeng, Cao Zhurong, Yu Xiaojin, Ye Wenhua, Zhen Wudi, Liu Jie, Wang Min, Jiang Shaoen, Pei Wenbing, Zhu Shaoping, Ding Yongkun, Zhang Weiyan, He Xiantu. Experimental analysis of indirect-drive ablative Rayleigh-Taylor instability on Shenguang Ⅱ[J]. High Power Laser and Particle Beams, 2015, 27(3): 032009.
[1] Lindl J D, Amendt P, Berger R L, et al. The physics basis for ignition using indirect-drive targets on the National Ignition Facility[J]. Phys Plasmas, 2004, 11: 339-491.
[2] Atzeni S, Meyer-ter-Vehn J. The Physics of Inertial Fusion: Beam Plasma Interaction Hydrodynamics, Hot Dense Mater[M]. Oxford: Oxford University, 2004.
[3] He X T, Zhang W Y. Inertial fusion research in China[J]. Eur Phys J D, 2007, 44: 227-231.
[4] Richtmyer R D. Taylor instability in shock acceleration of compressible fluids[J]. Commun Pre Appl Math, 1960, 13(2): 297-319.
[5] Meshkov E E. Instability of the interface of two gases accelerated by a shock wave[J]. Fluid Dyn, 1969, 4: 101-104.
[6] Rayleigh L. Investigation of the character of the equilibrium of an incompressible heavy fluid of variable density[J]. Proc London Math Soc, 1883, 14: 170-177.
[7] Taylor G I. The instability of liquid surfaces when accelerated in a direction perpendicular to their planes. (Ⅰ)[J]. Proc R Soc Lond A, 1950, 201: 192-196.
[8] Kull H. Incompressible description of Rayleigh-Taylor instabilities in laser-ablated plasmas[J]. Phys Fluids B, 1989, 1: 170-182.
[9] Ye W H, Zhang W Y, He X T. Stabilization of ablative Rayleigh-Taylor instability due to change of the Atwood number[J]. Phys Rev E, 2002, 65: 057401.
[10] Wang L F, Ye W H, He X T. Density gradient effects in weakly nonlinear ablative Rayleigh-Taylor instability[J]. Phys Plasmas, 2012, 19: 012706.
[11] Wang L F, Ye W H, Sheng Z M, et al. Preheating ablation effects on the Rayleigh-Taylor instability in the weakly nonlinear regime[J]. Phys Plasmas, 2010, 17: 122706.
[12] Wang L F, Ye W H, He X T, et al. Formation of jet-like spikes from the ablative Rayleigh-Taylor instability[J]. Phys Plasmas, 2012, 19: 100701.
[13] Ye W H, Wang L F, He X T. Spike deceleration and bubble acceleration in the ablative Rayleigh-Taylor instability[J]. Phys Plasmas, 2010, 17: 122704.
[14] Ye W H, Wang L F, He X T. Jet-like long spike in nonlinear evolution of ablative Rayleigh-Taylor instability[J]. Chin Phys Lett, 2012, 27: 125203.
[15] Ye W H, He X T, Zhang W Y. The effect of preheating on the nonlinear evolution of the ablative Rayleigh-Taylor instability[J]. Europhys Lett, 2011, 96: 35002.
[16] Guo H Y, Yu X J, Wang L F, et al. On the second harmonic generation through Bell-Plesset effects in cylindrical geometry[J]. Chin Phys Lett, 2014, 31: 044702.
[17] Regan S P, Epstein R, Hammel B A, et al. Hot-spot mix in ignition-scale inertial confinement fusion targets[J]. Phys Rev Lett, 2013, 111: 045001.
[18] Bodner S E. Rayleigh-Taylor instability and laser-pellet fusion[J]. Phys Rev Lett,1974, 33(13): 761-764.
[19] Takabe H, Mima K. Self-consistent growth rate of the Rayleigh-Taylor instability in an ablatively accelerating plasma[J]. Phys Fluids, 1985, 28: 3676-3682.
吴俊峰, 缪文勇, 王立锋, 曹柱荣, 郁晓瑾, 叶文华, 郑无敌, 刘杰, 王敏, 江少恩, 裴文兵, 朱少平, 丁永坤, 张维岩, 贺贤土. 神光Ⅱ装置上间接驱动烧蚀瑞利-泰勒不稳定性实验分析[J]. 强激光与粒子束, 2015, 27(3): 032009. Wu Junfeng, Miao Wenyong, Wang Lifeng, Cao Zhurong, Yu Xiaojin, Ye Wenhua, Zhen Wudi, Liu Jie, Wang Min, Jiang Shaoen, Pei Wenbing, Zhu Shaoping, Ding Yongkun, Zhang Weiyan, He Xiantu. Experimental analysis of indirect-drive ablative Rayleigh-Taylor instability on Shenguang Ⅱ[J]. High Power Laser and Particle Beams, 2015, 27(3): 032009.
PDF全文
