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Calculation of Direct Drive Targets for Megajoule Laser Facilities with Radiation in the Second and Third Harmonics of Nd Laser

机译:利用ND激光器第二和第三谐波辐射的Megajoule激光设施直接驱动目标计算

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The numerical results for cryogenic direct drive targets of megajoule facilities with radiation in the second and third harmonics of a Nd laser are presented. The calculations were performed with the 1D radiation hydrodynamics code ERA with the laser light absorption model that takes into account stimulated Brillouin scattering (SBS), generation of fast electrons in the processes of two-plasmon decay (TPD), and stimulated Raman scattering (SRS). The verification of the developed models was carried out on the basis of the comparison with experiments performed at the OMEGA and NIF facilities. The ignition margin (W-Q) of nonuniform fusion targets with an allowance for energy losses due to radiation transfer and heat conduction from the hot spot was the objective of the target optimization. The calculations showed that SBS and target heating by fast electrons generated in TPD and SRS fatally reduce W-Q of targets with a CH ablator for the megajoule laser with wavelength lambda = 0.53 mu m. The possibilities of decreasing these effects by replacing a CH ablator with a glass ablator and reducing the laser intensity upon increasing the target aspect ratio are considered. However, in both cases, W-Q remains substantially below unity for the laser with wavelength lambda = 0.53 mu m. The ignition margin increases by a factor of similar to 2 upon transition from the second to the third harmonic of a Nd laser. A glass ablator almost eliminates fast electrons in calculation with the laser wavelength lambda = 0.35 mu m. In this case, if SBS is reduced by a factor of 3-4 via shifting the laser emission lines in the neighboring channels by Delta mu approximate to 10-20 A, the ignition margin W-Q similar to 2 and a fusion energy yield of similar to 50 MJ are obtained in the 1D calculation for a laser energy of similar to 2 MJ and the third harmonic of a Nd laser.
机译:提出了具有ND激光器的第二和第三谐波中辐射的Megajoule设施的低温直接驱动目标的数值结果。用1D辐射流体动力学码时代进行计算,其中考虑到刺激的布里渊散射(SBS),在双量子衰减(TPD)的过程中产生快速电子的产生,并刺激拉曼散射(SRS )。基于与ω和NIF设施的实验的比较进行开发模型的验证。由于辐射转移和热点的热传导引起的不均匀融合目标的点火边缘(W-Q)具有占能量损失的余量是目标优化的目的。计算显示SBS和目标通过在TPD和SR中产生的快速电子加热,致命地减少具有用于波长λ=0.53μm的Megajoule激光的CH消烧器的靶标的W-Q。考虑了通过用玻璃烧蚀器替换CH消烧器并在增加目标纵横比时降低激光强度来降低这些效果的可能性。然而,在这两种情况下,W-Q对于具有波长λ=0.53μm的激光仍然基本上低于统一。从第二个激光器的第二次谐波转换时,点火边缘增加到2的倍数。玻璃烧蚀器几乎消除了使用激光波长λ=0.35μm的快速电子。在这种情况下,如果SBS通过ΔMu将相邻信道中的激光发射线近似为10-20a,则点火裕度wq类似于2的点火裕度wq和类似的融合能源产量在类似于2 MJ的激光能量和ND激光器的第三次谐波中获得50MJ。

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