非热等离子体中NO或活性氮的发射光谱分析

K. Shimizu, S. Saeki, G. Yamada, T. Oda
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引用次数: 3

摘要

由于放电等离子体处理受到气体组分的显著影响,为了了解活性物质的反应机理,采用了常压放电中的发射光谱法。利用数字控制谱仪和ICCD相机研究了N/sub 2/秒正带(SPB)、N/sub 2/一负带(FNB)和NO-/spl γ /带。当介电颗粒被放置在针板型电极之间时,这些发射沿电极轴减少。针板电极的正流光放电中,高能电子主要在针电极尖端周围产生,导致N/sub / 1负带。当放电能量超过一定值时,N/sub 2/第一负带的强度相对于其他带有所增加。这是由于针电极下方和介电板上存在高能电子。时间分辨率的发射光谱观测表明,N/sub 2/ s正带发射和N/sub 2/ 1负带发射在200 ns内消失,而NO-/spl γ /波段的发射持续时间超过3 /spl mu/s。这可能是由于发光机制的不同。N/sub - 2/第二正带和N/sub - 2/第一负带由电子碰撞激发,NO-/spl γ -带由N/sub - 2/(A)态分子碰撞激发。利用NO-/spl γ -/波段发射衰减常数,得到了NO分子在电晕放电和阻挡放电中的分布。在电晕放电中,NO可通过针尖处的还原反应被分解。相反,在阻挡放电中,NO可以通过板电极周围的还原反应被分解。
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Emission spectrometry of NO or activated nitrogen species in non-thermal plasma
Emission spectrometry in the atmospheric pressure discharge was carried out to understand reaction mechanisms of active species, as the discharge plasma processing is significantly influenced by the gas components. The N/sub 2/ second positive band (SPB), the N/sub 2/ first negative band (FNB) and the NO-/spl gamma/ band were investigated using a digital controlled spectrometer and an ICCD camera. When dielectric pellets were placed between a needle-plate type electrode, these emissions decreased along with the electrode axis. In the positive streamer discharges of needle-plate electrodes, high-energy electrons were mainly produced around the tip of the needle electrode leading to the N/sub 2/ first negative band. When the discharge energy exceeded a certain value, the intensity of the N/sub 2/ first negative band increased, compared to other bands. This is due to the presence of high-energy electrons below the needle electrode and on the dielectric plate. The emission spectrum observation with time resolution allowed us to conclude that the N/sub 2/ second positive band emission and that of N/sub 2/ first negative band emission were extinguished within 200 ns, while that of NO-/spl gamma/ band continued for more than 3 /spl mu/s. This could be due to a difference in the mechanisms of light emission. N/sub 2/ second positive band and N/sub 2/ first negative band were excited by electron collisions, while NO-/spl gamma/ band was energized by collisions of N/sub 2/(A)-state molecules. Distribution of NO molecules in the corona discharge or the barrier discharge was obtained from a decay constant of NO-/spl gamma/ band emission. NO could be decomposed by a reducing reaction at the tip of the needle in the corona discharge. On the contrary, NO could be decomposed by a reducing reaction around the plate electrode in the barrier discharge.
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