Plasma Density Influence on the Properties of a Plasma Filled Rod Pinch Diode

The rod pinch diode is perfect as a source of accelerators for flash X-ray radiography by virtue of a small and stable spot. But it is not suitable for intensive curreЦt drivers because of high diode impendence of 40~60Ω. However, by employing pre-filled plasma into diode prior to the driving curren...

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Published inPlasma science & technology Vol. 15; no. 9; pp. 904 - 907
Main Author 孙江 孙剑锋 杨海亮 张鹏飞 苏兆锋 周军
Format Journal Article
LanguageEnglish
Published 01.09.2013
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Summary:The rod pinch diode is perfect as a source of accelerators for flash X-ray radiography by virtue of a small and stable spot. But it is not suitable for intensive curreЦt drivers because of high diode impendence of 40~60Ω. However, by employing pre-filled plasma into diode prior to the driving current, the diode impendence can be effectively reduced. Plasma density plays an important role in this process, especially for sheath formation and space charge current in the diode. Analysis and simulation results show that a proper range of plasma density could be 1015~1016 cm-3.
Bibliography:SUN Jiang SUN Jianfeng YANG Hailiang ZHANG Pengfei. SU Zhaofeng ZHOU Jun( State Key Laboratory of Intense Pulsed Radiation Simulation and Effect, Northwest Institute of Nuclear Technology, Xi'an 710024, China)
plasma density, plasma filled rod pinch diode (PFRPD), sheath, space chargecurrent
34-1187/TL
The rod pinch diode is perfect as a source of accelerators for flash X-ray radiography by virtue of a small and stable spot. But it is not suitable for intensive curreЦt drivers because of high diode impendence of 40~60Ω. However, by employing pre-filled plasma into diode prior to the driving current, the diode impendence can be effectively reduced. Plasma density plays an important role in this process, especially for sheath formation and space charge current in the diode. Analysis and simulation results show that a proper range of plasma density could be 1015~1016 cm-3.
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ISSN:1009-0630
DOI:10.1088/1009-0630/15/9/14