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首页> 外文期刊>Laser and Particle Beams >Soft X-ray emissions from neon gas-puff Z-pinch powered by Qiang Guang-I accelerator
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Soft X-ray emissions from neon gas-puff Z-pinch powered by Qiang Guang-I accelerator

机译:强光一号加速器驱动的氖气Z型捏合器发出的软X射线

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The X-ray emission, especially the K-shell emission, from a neon gas-puff Z-pinch powered by the Qiang Guang-I accelerator, about 1.5 MA in amplitude and 100 ns in rise time, were calculated based on the two-level model and measured with X-ray diodes and an eight-frame X-ray pinhole camera. The simulation results showed that the K-shell yield is highly sensitive to the peak current. The experimental results confirmed that the matching of the Z-pinch load (mass and initial radius) to the current is crucial for getting a higher X-ray yield. Being determined by the imploding time, the pinch current plays a more important role than the current amplitude in K-shell emission. It seems that the preferable imploding time is about 110 ns. The K-shell radiation power with double shells, as a whole, is higher than that using single neon shell. While an implosion of a light (32 mg/cm) and small (20 mm in diameter) neon shell evolves with rather twist and asymmetries, a heavier (41 mg/cm) and bigger (25 mm in diameter) neon shell implodes more symmetrically. The double neon shells, 30 mm and 30 mg/cm for the outer shell, and 15-mm and 10 mg/cm for the inner shell, create almost “perfect” implosions evidenced by the early-time plasma shells with little perturbation and late stagnated pinch liners with a good axial uniformity. It was found that the “Zippering” effect leads to an earlier K-shell emission in the cathode region than that in the anode region, which extends the pulse width of K-shell emission.
机译:由强光I加速器驱动的氖气Z夹捏产生的X射线辐射,尤其是K壳发射,基于以下两个公式计算出:振幅约为1.5 MA,上升时间为100 ns水平模型,并使用X射线二极管和八幅X射线针孔照相机进行测量。仿真结果表明,K壳产量对峰值电流高度敏感。实验结果证实,Z捏负载(质量和初始半径)与电流的匹配对于获得更高的X射线产率至关重要。由内爆时间决定,收缩电流比K壳发射中的电流幅度更重要。似乎优选的内爆时间约为110 ns。整体上,具有双壳的K壳辐射功率高于使用单个霓虹壳的K壳辐射功率。轻(32 mg / cm)和小(直径20 mm)霓虹灯壳的内爆会以相当扭曲和不对称的形式发展,而较重(41 mg / cm)和更大(直径25 mm)的霓虹灯壳的内爆更加对称。双层霓虹灯外壳,外壳的厚度为30 mm和30 mg / cm,内壳的厚度为15 mm和10 mg / cm,产生了几乎“完美”的内爆,早期等离子外壳证明了这一点,几乎没有扰动,后期停滞的收缩衬套,具有良好的轴向均匀性。发现“拉链”效应导致在阴极区域中的K-壳发射比在阳极区域中的K-壳发射更早,这扩展了K-壳发射的脉冲宽度。

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