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Studies of electron energy distribution in plasma produced by a resonant laser pulse

机译:共振激光脉冲产生的等离子体中电子能量分布的研究

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摘要

Using the Langmuir probe method we evaluated the electron energy distribution (EED) in plasma produced in a Na+He mixture by a laser pulse tuned to the 3S-3P transition. We proposed a new method of retrieving the EED from the probe characteristics at high gas pressures, when the free path of the electrons is less than the probe radius, i.e. in the range of 2-100 Torr. The method consists of using a combination of the first and second derivatives of the electron current. The systematic error that usually occurs when the EED is treated by means of traditional Langmuir and diffusion probes was reduced by two to three times when treated this way. Two phase temporal evolution of the electron distribution was observed. Initially the shape of the EED was close to the Maxwellian function. Its temperature corresponded to the effective excitation temperature, which can characterize the total population of excited sodium atoms. When the concentration of excited atoms decreased, one observed a transformation of the EED function. At the second phase it became well Maxwellized only in the low energy region. The high energy part of the EED had a non-equilibrium shape. This was caused by relaxation of fast electrons produced by super-elastic collisions with residual excited atoms. [References: 35]
机译:使用Langmuir探针方法,我们通过调谐到3S-3P跃迁的激光脉冲评估了在Na + He混合物中产生的等离子体中的电子能量分布(EED)。我们提出了一种在电子的自由程小于探针半径(即2-100 Torr范围内)时在高气压下从探针特性中检索EED的新方法。该方法包括使用电子电流的一阶和二阶导数的组合。当用传统的Langmuir和扩散探头处理EED时,通常发生的系统误差减少了2到3倍。观察到电子分布的两相时间演变。最初,EED的形状接近麦克斯韦函数。它的温度对应于有效激发温度,该温度可以表征激发钠原子的总量。当激发原子的浓度降低时,人们观察到EED功能的转变。在第二阶段,仅在低能量区域内麦克斯韦化效果良好。 EED的高能部分具有非平衡形状。这是由于与残余激发原子发生超弹性碰撞而产生的快速电子弛豫引起的。 [参考:35]

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