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2017 Vol. 2, No. 2

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LASER- AND PARTICLE BEAM FUSION
Reviews
Optimization of laser illumination configuration for directly driven inertial confinement fusion
Murakami Masakatsu, Nishi Daiki
2017, 2(2) doi: 10.1016/j.mre.2016.12.002
Abstract:
Optimum laser configurations are presented to achieve high illumination uniformity with directly driven inertial confinement fusion targets. Assuming axisymmetric absorption pattern of individual laser beams, theoretical models are reviewed in terms of the number of laser beams, system imperfection, and laser beam patterns. Utilizing a self-organizing system of charged particles on a sphere, a simple numerical model is provided to give an optimal configuration for an arbitrary number of laser beams. As a result, such new configurations as “M48” and “M60” are found to show substantially higher illumination uniformity than any other existing direct drive systems. A new polar direct-drive scheme is proposed with the laser axes keeping off the target center, which can be applied to laser configurations designed for indirectly driven inertial fusion.
LASER- AND PARTICLE BEAM FUSION
First experimental comparisons of laser-plasma interactions between spherical and cylindrical hohlraums at SGIII laser facility
Chen Yaohua, Li Zhichao, Xie Xufei, Zheng Chunyang, Zhai Chuanlei, Hao Liang, Yang Dong, Huo Wenyi, Ren Guoli, Liu Jie, Peng Xiaoshi, Xu Tao, Li Yulong, Li Sanwei, Yang Zhiwen, Guo Liang, Hou Lifei, Liu Yonggang, Wei Huiyue, Liu Xiangming, Cha Weiyi, Li Yukun, Deng Keli, Yuan Zheng, Zhan Xiayu, Zhang Haijun, Jiang Baibin, Zhang Wei, Du Kai, Deng Xuewei, Ding Yongkun, Wei Xiaofeng, Zheng Wanguo, Chen Xiaodong, He Xiantu, Lan Ke
2017, 2(2) doi: 10.1016/j.mre.2017.01.001
Abstract:
We present our recent laser-plasmas instability (LPI) comparison experiment at the SGIII laser facility between the spherical and cylindrical hohlraums. Three kinds of filling are considered: vacuum, gas-filling with or without a capsule inside. A spherical hohlraum of 3.6 mm in diameter, and a cylindrical hohlraum of 2.4 mm × 4.3 mm are used. The capsule diameter is 0.96 mm. A flat-top laser pulse with 3 ns duration and up to 92.73 kJ energy is used. The experiment has shown that the LPI level in the spherical hohlraum is close to that of the outer beam in the cylindrical hohlraum, while much lower than that of the inner beam. The experiment is further simulated by using our 2-dimensional radiation hydrodynamic code LARED-Integration, and the laser back-scattering fraction and the stimulated Raman scatter (SRS) spectrum are post-processed by the high efficiency code of laser interaction with plasmas HLIP. According to the simulation, the plasma waves are strongly damped and the SRS is mainly developed at the plasma conditions of electron density from 0.08 nc to 0.1 nc and electron temperature from 1.5 keV to 2.0 keV inside the hohlraums. However, obvious differences between the simulation and experiment are found, such as that the SRS back-scattering is underestimated, and the numerical SRS spectrum peaks at a larger wavelength and at a later time than the data. These differences indicate that the development of a 3D radiation hydrodynamic code, with more accurate physics models, is mandatory for spherical hohlraum study.
Reviews
Laser-direct-drive program: Promise, challenge, and path forward
Campbell E.M., Goncharov V.N., Sangster T.C., Regan S.P., Radha P.B., Betti R., Myatt J.F., Froula D.H., Rosenberg M.J., Igumenshchev I.V., Seka W., Solodov A.A., Maximov A.V., Marozas J.A., Collins T.J.B., Turnbull D., Marshall F.J., Shvydky A., Knauer J.P., McCrory R.L., Sefkow A.B., Hohenberger M., Michel P.A., Chapman T., Masse L., Goyon C., Ross S., Bates J.W., Karasik M., Oh J., Weaver J., Schmitt A.J., Obenschain K., Obenschain S.P., Reyes S., Van Wonterghem B.
2017, 2(2) doi: 10.1016/j.mre.2017.03.001
Abstract:
Along with laser-indirect (X-ray)-drive and magnetic-drive target concepts, laser direct drive is a viable approach to achieving ignition and gain with inertial confinement fusion. In the United States, a national program has been established to demonstrate and understand the physics of laser direct drive. The program utilizes the Omega Laser Facility to conduct implosion and coupling physics at the nominally 30-kJ scale and laser–plasma interaction and coupling physics at the MJ scale at the National Ignition Facility. This article will discuss the motivation and challenges for laser direct drive and the broad-based program presently underway in the United States.
LASER- AND PARTICLE BEAM FUSION
P2 asymmetry of Au's M-band flux and its smoothing effect due to high-Z ablator dopants
Li Yongsheng, Zhai Chuanlei, Ren Guoli, Gu Jianfa, Huo Wenyi, Meng Xujun, Ye Wenhua, Lan Ke, Zhang Weiyan
2017, 2(2) doi: 10.1016/j.mre.2016.12.001
Abstract:
X-ray drive asymmetry is one of the main seeds of low-mode implosion asymmetry that blocks further improvement of the nuclear performance of “high-foot” experiments on the National Ignition Facility [Miller et al., Nucl. Fusion 44, S228 (2004)]. More particularly, the P2 asymmetry of Au's M-band flux can also severely influence the implosion performance of ignition capsules [Li et al., Phys. Plasmas 23, 072705 (2016)]. Here we study the smoothing effect of mid- and/or high-Z dopants in ablator on Au's M-band flux asymmetries, by modeling and comparing the implosion processes of a Ge-doped ignition capsule and a Si-doped one driven by X-ray sources with P2 M-band flux asymmetry. As the results, (1) mid- or high-Z dopants absorb hard X-rays (M-band flux) and re-emit isotropically, which helps to smooth the asymmetric M-band flux arriving at the ablation front, therefore reducing the P2 asymmetries of the imploding shell and hot spot; (2) the smoothing effect of Ge-dopant is more remarkable than Si-dopant because its opacity in Au's M-band is higher than the latter's; and (3) placing the doped layer at a larger radius in ablator is more efficient. Applying this effect may not be a main measure to reduce the low-mode implosion asymmetry, but might be of significance in some critical situations such as inertial confinement fusion (ICF) experiments very near the performance cliffs of asymmetric X-ray drives.