The emission characteristics of afterglow in a microsecond pulsed glow discharge atomic source are studied to obtain insight into the excitation and recombination processes of analytes and fill gases. Each emission line features an initial intense peak at the beginning of the discharge pulse. The afterglow, which has been observed in the temporal behavior for some emission temporal profiles of analytes and discharge gases, exhibits an intense post-pulse signal maximized at 25-35 mu s after plasma termination, with a broader profile than their initial peaks. The afterglow of Ar I and Cu I spectra last approximately 100 mu s and 300 mu s, respectively, after the argon discharge pulse at 2.0 torr pressure. The intensity of the afterpeak increases with the pulse width between 2 mu s to 200 mu s. A study of fourteen Ar I and twenty-seven Cu I lines show that transitions from high energy levels (5p[ 14.5-14.7 eV] for Ar and above 6 eV for Cu) are relatively stronger in the afterglow. The highly excited argon and copper atoms are thought to be generated via the recombination of ions and electrons. The results are explained primarily in terms of an electron-electron-ion three-body recombination process.
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机译:研究了微秒脉冲辉光放电原子源中余辉的发射特性,以深入了解分析物和填充气体的激发和复合过程。每条发射线在放电脉冲开始时都有一个初始的强烈峰值。在分析物和放电气体的某些发射时间曲线的时间行为中观察到的余辉,显示出强烈的脉冲后信号,在等离子终止后在25-35 s s处最大,其轮廓比其初始峰值更宽。在2.0托压力下的氩气放电脉冲之后,Ar I和Cu I光谱的余辉分别持续约100μs和300μs。后峰的强度随着2 s到200 s s之间的脉冲宽度而增加。对14条Ar I和27条Cu I线的研究表明,在余辉中,高能级(Ar的5p [14.5-14.7 eV]和Cu的6 eV以上)的跃迁相对较强。据认为,高激发氩和铜原子是通过离子和电子的复合而产生的。主要根据电子-电子-离子三体复合过程来解释结果。
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