Micro hollow cathode discharges (MHCD) were produced using 250 m thickdielectric layer of alumina sandwiched between two nickel electrodes of 8 mthickness. A through cavity at the center of the chip was formed by laserdrilling technique. MHCD with a diameter of few hundreds of micrometers allowedus to generate direct current discharges in helium at up to atmosphericpressure. A slowly varying ramped voltage generator was used to study theignition and the extinction periods of the microdischarges. The analysis wasperformed by using electrical characterisation of the V-I behaviour and themeasurement of He*(3S1) metastable atoms density by tunable diode laserspectroscopy. At the ignition of the microdischarges, 2 s long current peak ashigh as 24 mA was observed, sometimes followed by low amplitude dampedoscillations. At helium pressure above 400 Torr, an oscillatory behaviour ofthe discharge current was observed just before the extinction of themicrodischarges. The same type of instability in the extinction period at highpressure also appeared on the density of He*(3S1) metastable atoms, but delayedby a few s relative to the current oscillations. Metastable atoms thus cannotbe at the origin of the generation of the observed instabilities.
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机译:使用夹在两个厚度为8 m的镍电极之间的250 m厚的氧化铝介电层,可产生微空心阴极放电(MHCD)。通过激光钻孔技术在芯片中心形成通孔。直径为几百微米的MHCD可以在高达大气压的氦气中产生直流电。使用缓慢变化的斜坡电压发生器来研究微放电的着火和熄灭时间。利用V-I行为的电学表征和可调谐二极管激光光谱法测量He *(3S1)亚稳原子密度进行了分析。在点燃微放电时,观察到2 s长的电流峰值,高达24 mA,有时还会出现低幅度的阻尼振荡。在氦气压力高于400 Torr时,恰好在微放电消失之前观察到放电电流的振荡行为。 He *(3S1)亚稳原子的密度上也出现了相同的类型的灭绝高压不稳定性,但相对于电流振荡延迟了几秒。因此,亚稳态原子不能处在观察到的不稳定性产生的起点。
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