用激光诱导荧光在氩等离子体中测量磁化预护套

M. U. Siddiqui, N. Hershkowitz
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摘要

只提供摘要形式。经典的玻姆准则只对未磁化的弱碰撞等离子体有效。对于磁场斜入射到边界的磁化等离子体,Chodura和后来的Riemann声称,预鞘层沿着磁力线加速离子到声速。在此之后,必须存在一个额外的“磁性预鞘”,它与离子陀螺半径成比例,并沿着磁力线加速离子从声速到垂直于边界的声速。Riemann和Franklin声称前鞘和磁性前鞘都有一个单一的结构。以前的实验试图通过测量等离子体电位结构来验证鞘前尺度长度,但没有实际测量离子流速,因此它们的鞘前长度没有得到适当的定义。Kim等人发现,在磁化和碰撞等离子体中,预鞘层有两种不同的势结构,一种是随离子碰撞长度缩放的,另一种是随离子陀螺半径缩放的,这与Riemann和Franklin的说法相反。在这项工作中,作者研究了感应氩等离子体中的磁性和碰撞鞘前尺度长度,使用激光诱导荧光测量离子流动速度,从而确定鞘前边界。与Chodura、Riemann和Franklin提出的理论进行了比较。
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Measurement of magnetized presheaths using laser-induced fluorescence in argon plasmas
Summary form only given. The classic Bohm's Criterion is valid only for unmagnetized, weakly-collisional plasmas. For magnetized plasmas where the magnetic field is obliquely incident to the boundary, Chodura and later Riemann, claimed that the presheath, accelerates ions to the sound speed along the magnetic field lines. After this an additional “magnetic presheath” must exist, which scales with the ion gyro radius, and accelerates the ions from the sound speed along the magnetic lines of force, to the sound speed perpendicular to the boundary. Riemann and Franklin claimed that both the presheath and magnetic presheath had a single structure. Previous experiments attempted to verify the presheath scale lengths by measuring plasma potential structures, however none actually measured ion flow velocity, and as such their presheath lengths were not properly defined. Kim et. al. found that in magnetized and collisional plasmas, the presheaths had two distinct potential structures, one that scaled with the ion collision length and on that scaled with the ion gyro radius, contrary to Riemann and Franklin's claims. In this work the authors investigate magnetic and collisional presheath scale lengths in an inductive Argon plasma, using laser-induced fluorescence to measure ion flow speed thus and define the presheath boundaries. The scale lengths and presheath potential structures are compared to theory presented by Chodura, Riemann and Franklin.
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