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Neutron emission generated during wire array Z-pinch implosion onto deuterated fiber

机译:线阵列Z捏爆合到氘代光纤上时产生的中子发射

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摘要

The implosion of both cylindrical and conical wire arrays onto a deuterated polyethylene fiber was studied on the S-300 pulsed power generator [A. S. Chernenko et al., Proceedings of the 11th International Conference on High Power Particle Beams (Academy of Science of Czech Republic, Prague, 1996), p. 154]. Neutron measurements were used to obtain information about acceleration of fast deuterons. An average neutron yield approached 109 on the current level of 2 MA. In the case of conical wire arrays, side-on neutron energy spectra peaked at 2.48 +/- 0.05 MeV with 450 +/- 100 keV full width at half-maximum. In the downstream direction, the peak neutron energy and the width of a neutron spectrum were 2.65 +/- 0.10 MeV and 350 +/- 100 keV, respectively. The total number of fast deuterons was 1015 and their average kinetic energy was about 150 keV. Most of the deuterons were directed toward the cathode. The broad width of neutron spectra in the side-on direction implied a high radial component of deuteron velocity. With regard to the emission time, neutron pulses temporally correlated with hard x rays and also with measured voltage. The neutron emission lasted on average 30 +/- 5 ns and it was observed during the stagnation and at the beginning of the expansion of a plasma column. At this moment, the plasma impedance reached 0.2-0.4 Omega. In the post-stagnation phase, this value was formed significantly by enhanced plasma resistance. Similar experimental results were observed also with cylindrical wire arrays imploding onto a deuterated fiber. (C) 2008 American Institute of Physics.
机译:在S-300脉冲发电机上研究了圆柱形和锥形线阵列在氘化聚乙烯纤维上的内爆[A. S. Chernenko等人,《第十一届国际高功率粒子束会议论文集》(捷克共和国科学院,布拉格,1996年),第1页。 154]。中子测量用于获得有关快氘核加速的信息。在当前的2 MA水平下,平均中子产率接近109。在圆锥形线阵列的情况下,侧向中子能谱在2.48 +/- 0.05 MeV处达到峰值,全宽为450 +/- 100 keV,一半为最大值。在下游方向,中子的峰值能量和中子谱的宽度分别为2.65 +/- 0.10 MeV和350 +/- 100 keV。快速氘核的总数为1015,其平均动能约为150 keV。大部分氘核都指向阴极。中子光谱在横向方向上的较宽宽度意味着氘核速度具有较高的径向分量。关于发射时间,中子脉冲在时间上与硬X射线以及所测量的电压相关。中子发射平均持续30 +/- 5 ns,在停滞期间和等离子柱膨胀开始时观察到。此时,等离子体阻抗达到0.2-0.4Ω。在停滞后阶段,该值是由增强的等离子体电阻显着形成的。当圆柱线阵列插入氘化纤维上时,也观察到类似的实验结果。 (C)2008美国物理研究所。

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