纳秒
电场
材料科学
阴极
电离
原子物理学
电介质
拉曼散射
介质阻挡放电
汤森排放
拉曼光谱
分子物理学
光电子学
离子
光学
物理
激光器
化学
物理化学
量子力学
作者
Tsuyohito Ito,Tatsuya Kanazawa,Satoshi Hamaguchi
标识
DOI:10.1103/physrevlett.107.065002
摘要
The discharge initiation mechanism of nanosecond dielectric barrier discharges in open air has been clarified with time-dependent measurement of the discharge electric field by electric-field-induced coherent Raman scattering and optical emission. Our experimental observations have revealed that, in the prebreakdown phase of a nanosecond dielectric barrier discharge, the externally applied fast-rising electric field is strongly enhanced near the cathode due to large accumulation of space charge, which then strongly enhances ionization near the cathode. Once a sufficiently large number of ionizations take place, the location of peak ionization forms a front and propagates toward the cathode with strong optical emission, which establishes the discharge. This process is essentially different from the well-known Townsend mechanism for slower discharges.
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