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Laser beam propagation through inertial confinement fusion hohlraum plasmas

机译:激光束通过惯性约束聚变等离子体的传播

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摘要

A study of the laser-plasma interaction processes have been performed in plasmas that are created to emulate the plasma conditions in indirect drive inertial confinement fusion targets. The plasma emulator is produced in a gas-filled hohlraum+ADs- a blue 351-nm laser beam propagates along the axis of the hohlraum interacting with a high-temperature (Te+AD0- 3.5 keV), dense (ne+AD0- 5 x 10(20) cm(-3)), long-scale length (L - 2 mm ) plasma. Experiments at these conditions have demonstrated that the interaction beam produces less than 1+ACU- total backscatter resulting in transmission greater than 90+ACU- for laser intensities less than I +ADw- 2 x 1015 W cm(-2). The bulk plasma conditions have been independently characterized using Thomson scattering where the peak electron temperatures are shown to scale with the hohlraum heater beam energy in the range from 2 keV to 3.5 keV. This feature has allowed us to determine the thresholds for both backscattering and filamentation instabilities+ADs- the former measured with absolutely calibrated full aperture backscatter and near backscatter diagnostics and the latter with a transmitted beam diagnostics. Comparing the experimental results with detailed gain calculations for the onset of significant laser scattering processes shows a stimulated Brillouin scattering threshold (R+AD0- 10+ACU-) for a linear gain of 15+ADs- these high temperature, low density experiments produce plasma conditions comparable to those along the outer beams in ignition hohlraum designs. By increasing the gas fill density (ne+AD0- 1021 cm(-3)) in these targets, the inner beam ignition hohlraum conditions are accessed. In this case, stimulated Raman scattering dominates the backscattering processes and we show that scattering is small for gains less than 20 which can be achieved through proper choice of the laser beam intensity. (C) 2007 American Institute of Physics.
机译:已经在等离子体中进行了激光-等离子体相互作用过程的研究,该等离子体模拟了间接驱动惯性约束聚变靶中的等离子体条件。等离子体模拟器是在充满气体的hohlraum + ADs中产生的-351 nm的蓝色激光束沿着hohlraum的轴传播,并与高温(Te + AD0- 3.5 keV)致密(ne + AD0-5 x 10(20)cm(-3)),长标度(L-2 mm)等离子。在这些条件下的实验表明,对于激光强度小于I + ADw-2 x 1015 W cm(-2)的激光,相互作用光束产生的总背向散射小于1 + ACU-,导致透射大于90 + ACU-。整体等离子体条件已使用汤姆森散射进行了独立表征,其中峰值电子温度显示为与球形加热器束能量在2 keV至3.5 keV范围内成比例。此功能使我们能够确定后向散射和灯丝不稳定性+ ADs的阈值-前者是使用绝对校准的全孔径后向散射和近后向散射诊断来测量的,后者是通过透射束诊断来测量的。将实验结果与详细的增益计算进行比较,以得出重要的激光散射过程的开始,表明线性增益为15 + ADs时受激布里渊散射阈值(R + AD0-10 + ACU-),这些高温,低密度实验会产生等离子体的条件与点火炉设计中沿外梁的条件相当。通过增加这些目标中的气体填充密度(ne + AD0-1021 cm(-3)),可以访问内部光束点火角度条件。在这种情况下,受激拉曼散射在反向散射过程中占主导地位,我们表明,对于小于20的增益,散射很小,这可以通过适当选择激光束强度来实现。 (C)2007美国物理研究所。

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