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Ecton processes in the generation of pulsed runaway electron beams in a gas discharge

机译:在气体放电中产生脉冲失控电子束的切割过程

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As was shown earlier for pulsed discharges that occur in electric fields rising with extremely high rates (10(18) V/(cm s)) during the pulse rise time, the electron current in a vacuum discharge is lower than the current of runaway electrons in an atmospheric air discharge in a 1-cm-long gap. In this paper, this is explained by that the field emission current from cathode microprotrusions in a gas discharge is enhanced due to gas ionization. This hastens the initiation of explosive electron emission, which occurs within 10(-11) s at a current density of up to 10(10) A/cm(2). Thereafter, a first-type cathode spot starts forming. The temperature of the cathode spot decreases due to heat conduction, and the explosive emission current ceases. Thus, the runaway electron current pulse is similar in nature to the ecton phenomenon in a vacuum discharge.
机译:如前所述,对于在脉冲升高期间以极高的速率上升(10(18)v /(cm s)上升的电场中发生的脉冲放电,真空放电中的电子电流低于失控电子的电流 在一个大气压的空气中,在1厘米长的间隙中。 在本文中,通过气体离子化而增强来自气体排放中的阴极微胶凝的场发射电流来解释。 这使得爆炸性电子发射的开始,其在10(-11)秒内发生高达10(10)/ cm(2)的电流密度。 此后,第一型阴极点开始形成。 阴极点的温度由于热传导而降低,并且爆炸发射电流停止。 因此,失控的电子电流脉冲本质上与真空放电中的省份现象类似。

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