期刊文献+

A new ignition hohlraum design for indirect-drive inertial confinement fusion 被引量:1

A new ignition hohlraum design for indirect-drive inertial confinement fusion
下载PDF
导出
摘要 In this paper,a six-cylinder-port hohlraum is proposed to provide high symmetry flux on capsule.It is designed to ignite a capsule with 1.2-mm radius in indirect-drive inertial confinement fusion(ICF).Flux symmetry and laser energy are calculated by using three-dimensional view factor method and laser energy balance in hohlraum.Plasma conditions are analyzed based on the two-dimensional radiation-hydrodynamic simulations.There is no Y_(lm)(l≤4) asymmetry in the six-cylinder-port hohlraum when the influences of laser entrance holes(LEHs) and laser spots cancel each other out with suitable target parameters.A radiation drive with 300 eV and good flux symmetry can be achieved by using a laser energy of 2.3 MJ and peak power of 500 TW.According to the simulations,the electron temperature and the electron density on the wall of laser cone are high and low,respectively,which are similar to those of outer cones in the hohlraums on National Ignition Facility(NTF).And the laser intensity is also as low as those of NIF outer cones.So the backscattering due to laser plasma interaction(LPI) is considered to be negligible.The six-cyliner-port hohlraum could be superior to the traditional cylindrical hohlraum and the octahedral hohlraum in both higher symmetry and lower backscattering without supplementary technology at an acceptable laser energy level.It is undoubted that the hohlraum will add to the diversity of ICF approaches. In this paper,a six-cylinder-port hohlraum is proposed to provide high symmetry flux on capsule.It is designed to ignite a capsule with 1.2-mm radius in indirect-drive inertial confinement fusion(ICF).Flux symmetry and laser energy are calculated by using three-dimensional view factor method and laser energy balance in hohlraum.Plasma conditions are analyzed based on the two-dimensional radiation-hydrodynamic simulations.There is no Y_(lm)(l≤4) asymmetry in the six-cylinder-port hohlraum when the influences of laser entrance holes(LEHs) and laser spots cancel each other out with suitable target parameters.A radiation drive with 300 eV and good flux symmetry can be achieved by using a laser energy of 2.3 MJ and peak power of 500 TW.According to the simulations,the electron temperature and the electron density on the wall of laser cone are high and low,respectively,which are similar to those of outer cones in the hohlraums on National Ignition Facility(NTF).And the laser intensity is also as low as those of NIF outer cones.So the backscattering due to laser plasma interaction(LPI) is considered to be negligible.The six-cyliner-port hohlraum could be superior to the traditional cylindrical hohlraum and the octahedral hohlraum in both higher symmetry and lower backscattering without supplementary technology at an acceptable laser energy level.It is undoubted that the hohlraum will add to the diversity of ICF approaches.
出处 《Chinese Physics B》 SCIE EI CAS CSCD 2016年第8期256-260,共5页 中国物理B(英文版)
基金 supported by the National Natural Science Foundation of China(Grant Nos.11435011 and 11575034)
关键词 ICE hohlraums IGNITION six-cylinder port ICE hohlraums, ignition, six-cylinder port
  • 相关文献

参考文献18

  • 1Lindl J D, Amendt P, Berger R L, Glendinning S G, Glenzer S H, Haan S W, Kauffman R L, Landen O L and Suter L J 2004 Phys. Plasmas 2 3933.
  • 2Atzeni S and Meyer-ter-Vehn J 2004 The Physics of Inertial Fusion (Oxford:Oxford Science Press).
  • 3Haan S W, Lindl J D, Callanhan D A, Clark D S, Salmonson J D, Hammel B A, Atherton L J, Cook R C, Edwards M J, Glenzer S, Hamza A V, Hatchett S P, Herrmann M C, Hinkel D E, Ho D D, Huang H, Jones O S, Kline J, Kyrala G, Lanen O L, MacGowan B J, Marinak M M, Meyerhofer D D, Milovich J L, Moreno K A, Moses E I, Munro D H, Nikroo A, Olson R E, Peterson K, Pollaine S M, Ralph J E, Robey H F, Spears B K, Springer P T, Suter L J, Thomas C A, Town R P, Vesey R, Weber S V, Wilkens H L and Wilson D C 2011 Phys. Plasmas 18 051001.
  • 4Phillion D W and Pollaine S M 1994 Phys. Plasmas 1 2963.
  • 5Schnittman J D and Craxton R S 1996 Phys. Plasmas 3 3786.
  • 6Lan K, Liu J, Lai D X, Zheng W D and He X T 2014 Phys. Plasmas 21 010704.
  • 7Lan K, He X T, Liu J, Zheng W D and Lai D X 2014 Phys. Plasmas 21 052704.
  • 8Lan K and Zheng W D 2014 Phys. Plasmas 21 090704.
  • 9Kyrala G A, Kline J L, Dixit S, Glenzer S, Kalantar D, Bradley D, Lzumi N, Meezan N, Landen O, Callahan D, Weber S V, Holder J P, Glenn S, Edwards M J, Koch J, Suter L J, Haan S W, Town R P J, Michel P, Jones O, Langer S, Moody J D, Dewald E L, Ma T, Ralph J, Hamza A, Dzenitis E and Kilkenny J 2011 Phys. Plasmas 18 056307.
  • 10Michel P, Glenzer S H, Divol L, Bradley D K, Callahan D, Dixit S, Glenn S, Hinkel D, Kirkwood R K, Kline J L, Kruer W L, Kyrala G A, LePage S, Meezan N B, Town R, Widmann K, Williams E A, MacGowan B J, Lindl J and Suter L J 2010 Phys. Plasmas 17 056305.

同被引文献15

引证文献1

  • 1李三伟,杨冬,李欣,李志超,郭亮,谢旭飞,况龙钰,张璐,霍文义,吴畅书,陈耀桦,宋鹏,张桦森,曹柱荣,胡昕,侯立飞,易荣清,蒋小华,李琦,宋天明,彭晓世,徐涛,理玉龙,邓博,邓克立,王强强,杨品,黎航,袁铮,魏惠月,刘祥明,查为懿,刘永刚,王哲斌,章欢,詹夏宇,陈黎,梅雨,陈韬,李晋,杨志文,杜华冰,车兴森,杨轶蒙,杨正华,景龙飞,何小安,李朝光,王鹏,于瑞珍,苏春晓,陈铭,崔延莉,王峰,刘慎业,杨家敏,江少恩,张保汉,蓝可,古培俊,邹士阳,郑无敌,刘杰,丁永坤.我国激光间接驱动黑腔物理实验研究进展[J].中国科学:物理学、力学、天文学,2018,48(6):3-20. 被引量:6

二级引证文献6

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部