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Contribution of the backstreaming ions to the self-magnetic pinch (SMP) diode current

机译:后游离子对自磁夹(SMP)二极管电流的贡献

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The results presented here were obtained with a self-magnetic pinch (SMP) diode mounted at the front high voltage end of the RITS accelerator. RITS is a Self-Magnetically Insulated Transmission Line (MITL) voltage adder that adds the voltage pulse of six 1.3 MV inductively insulated cavities. The RITS driver together with the SMP diode has produced x-ray spots of the order of 1 mm in diameter and doses adequate for the radiographic imaging of high area density objects. Although, through the years, a number of different types of radiographic electron diodes have been utilized with SABER, HERMES III and RITS accelerators, the SMP diode appears to be the most successful and simplest diode for the radiographic investigation of various objects. Our experiments had two objectives: first to measure the contribution of the back-streaming ion currents emitted from the anode target and second to try to evaluate the energy of those ions and hence the Anode-Cathode (A-K) gap actual voltage. In any very high voltage inductive voltage adder utilizing MITLs to transmit the power to the diode load, the precise knowledge of the accelerating voltage applied on the A-K gap is problematic. This is even more difficult in an SMP diode where the A-K gap is very small (similar to 1 cm) and the diode region very hostile. The accelerating voltage quoted in the literature is from estimates based on the measurements of the anode and cathode currents of the MITL far upstream from the diode and utilizing the para-potential flow theories and inductive corrections. Thus, it would be interesting to have another independent measurement to evaluate the A-K voltage. The diode's anode is made of a number of high-Z metals in order to produce copious and energetic flash x-rays. It was established experimentally that the back-streaming ion currents are a strong function of the anode materials and their stage of cleanness. We have measured the back-streaming ion currents emitted from the anode and propagat
机译:这里呈现的结果是用安装在射线加速器的前高压端的自磁夹(SMP)二极管获得。射灯是一种自磁绝缘的传输线(MITL)电压加法器,其增加了六个1.3 mV电感绝缘腔的电压脉冲。与SMP二极管一起具有直径为1mm的X射线斑点,并且剂量适用于高面积密度对象的射线影像。虽然多年来,许多不同类型的放射线电子二极管已经被Saber,Hermes III和RIS型加速器使用,但SMP二极管似乎是用于各种物体的放射线照相调查的最成功和最简单的二极管。我们的实验有两个目的:首先测量从阳极靶发出的背流离子电流的贡献,并将其次尝试评估这些离子的能量,从而评估阳极 - 阴极(A-K)间隙实际电压。在利用MITLS将电力传输到二极管负载的任何非常高的电感电压加法器中,在A-K间隙上施加的加速电压的精确知识是有问题的。这在SMP二极管中更加困难,其中A-K间隙非常小(类似于1cm)和二极管区域非常敌对。文献中引用的加速电压来自估计基于二极管上游的阳极和阴极电流的测量,并利用Para潜在的流动理论和电感校正。因此,具有另一个独立的测量来评估A-K电压将是有趣的。二极管的阳极由许多高Z金属制成,以产生丰富和精力充沛的闪光X射线。实验地建立了后流离子电流是阳极材料的强函数及其清洁阶段。我们测量了从阳极和繁荣发射的后流离子电流

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