期刊文献+

用于快点火的激光驱动器组束方式 被引量:1

Laser driver beam combination for fast ignition
下载PDF
导出
摘要 根据实现快点火激光的预估参数要求,分析了非相干组束和相干组束是否可满足快点火所需的激光功率密度和能量。引入与实际情况相当的畸变波前分析远场焦斑,为了满足能量要求非相干组束需要组合更多的光束,并改进驱动器的稳定性将角漂控制在±2μrad范围内;相干组束可获得更小的焦斑有利于提高功率密度,同时可降低对能量的要求,但仅对单路光分别进行波前补偿并不能提高能量集中度,需要引入复杂的监测和控制设备对整个通光孔径内的波前(包括束内和束间)进行全局控制。基于目前提出的参数要求和波前校正能力,非相干合成更易实现快点火,但相干合成则具有更广泛的应用潜力。 Based on the estimated parameters of fast ignition,the requirements for laser-beam power intensity and energy are used to analyze the possibility of realizing fast ignition by coherent combination and non-coherent combination.The practical distorted wavefront is considered to analyze the far-field focal spot.Non-coherent combination needs more beams for energy requirement and to limit angle drifting in ±2 μrad through improving laser driver's stability.Coherent combination is beneficial for achieving smaller focal spot and higher power intensity,simultaneously reducing the requirement of energy,but single beam wavefront correction can not improve the power intensity in this method,which leads to combined wavefront correction of the total clear aperture with complex monitoring and control methods.Based on the requirement of parameters and wavefront correction capability,non-coherent beam combination is easier to achieve for fast ignition,however,coherent beam combination has the potential for extensive application.
出处 《强激光与粒子束》 EI CAS CSCD 北大核心 2011年第3期697-701,共5页 High Power Laser and Particle Beams
基金 国家高技术发展计划项目 激光聚变实验室和激光研究中心创新基金项目
关键词 快点火 非相干组束 相干组束 波前误差 功率密度 fast ignition non-coherent combination coherent combination wavefront error power intensity
  • 相关文献

参考文献17

  • 1Tabak M, Hammer J, Michael E. Ignition and high gain with ultra powerful lasers[J]. PhysPlasmas, 1994, 1(50): 1626-1634.
  • 2Gibbon P, Foster E. Shortpulse laserplasma interaction[J]. Phys Control Fusion, 1996, 38:7769-7793.
  • 3Bastiani S, Rosusse A, Geindre J P, et al. Experiment study of the interaction of subpicosecond laser pulses with solid targets of varying initial scale lengths[J]. PhysRev E, 1997, 56(6): 7179-7185.
  • 4Zhang P, He J T, Chen D B, et al. Effects of a prepulse on Yray radiation produced by afemtosecond laser with only 5 mJ energy[J]. PhysRev E,1998,57(4):3746-3748.
  • 5Rousseaux C, Amiranoff F, Labaune (7, et al. Suprathermal and relativistic electrons produced in laserplasma interaction at 0.26, 0.53 and 1.05 pm laser wavelength[J]. PhysFluids B, 1992, 4(8) :2589-2595.
  • 6李业军,路建新,王雷剑,黄永盛,张骥,张海峰,汤秀章.超短脉冲激光与固体等离子体相互作用实验研究[J].原子能科学技术,2008,42(12):1082-1085. 被引量:3
  • 7Miyanaga N, Azechi H, Jitsuno T, et al. Development of 10kJ PW laser for the FIREX-I program[J]. Journal de physique IV, 2006, 133 (1):81-87.
  • 8Miyanaka M, Azechi H, Tanaka K A, et al. FIREX petawatt laser development for fast ignition research at 1LE[C]//Proceedings of Inertial Science and Applications. 2003:507-511.
  • 9John K C. Integrating four, highenergy, petawatt beamlines into the National Ignition Facility[R]. The 3rd Internatinoal Conference on Ultrahigh Intensity Lasers(ICUIL), 2008.
  • 10Micheal H K. Fast ignition[R]. LLNL PRES-415135, 2009.

二级参考文献25

  • 1朱燕堂 赵选民 等.应用概率统计方法[M].西安:西北工业大学出版社,2000..
  • 2TABAK M, HAMMER J, GLINSKY M E, et al. Ignition and high gain with ultrapowerful lasers[J]. Phys Plasmas, 1994, 1(5): 1 626-1 634.
  • 3GIBBON P, FOSTER E. Short-pulse laserplasmas interaction plasma [J]. Phys Control Fusion, 1996, 38, 7 769-7 793.
  • 4BASTIANI S, ROSUSSE A, GEINDRE J P, et al. Experiment study of the interaction of subpicosecond laser pulses with solid targets of varying initial scale lengths[J]. Phys Rev E, 1997, 56 (6):7 179-7 185.
  • 5ZHANG P, HE J T, Chen D B, et al. Effects of a pre-pulse on 7-ray radiation produced by a femtosecond laser with only 5 mJ energy[J]. Phys Rev E, 1998, 57(4): 3 746-3 748.
  • 6ROUSSEAUX C, AMIRANOFF F, LABAUNE C, et al. Suprathermal and relativistic electrons produced in laser-plasma interaction at 0. 26, 0.53, and 1.05 μm laser wavelength[J]. Phys Fluids B, 1992, 4(8): 2 589-2 595.
  • 7MALKA G, MIQUEL J L. Experimental confirmation of ponderomotive-force electrons produced by an ultrarelativistic laser pulse on a solid target [J]. PhysRevLett, 1996, 77(1): 75-78.
  • 8ROUSSE A, AUDEBERT P, GEINDRE J P, et al. Efficient K, X-ray source from femtosecond laser-produced plasmas[J]. Phys Rev E, 1994, 50(3): 2 200-2 207.
  • 9FEWS A P, NORREYS P A, BEG F N, et al Plasma ion emission from high intensity picosecond laser pulse interactions with solid targets[J]. Phys Rev Lett, 1994, 73(13):1 801-1 804.
  • 10SCHNURER M, KALASHNIKOV M P, NICKLES P V. Hard X-ray emission from intense short pulse laser plasmas[J]. Phys Plasmas, 1995, 2(8): 3 106-3 110.

共引文献9

同被引文献18

引证文献1

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