{"title":"On double-layer and reverse discharge creation during long positive voltage pulses in a bipolar HiPIMS discharge","authors":"A D Pajdarová, T Kozák, T Tölg and J Čapek","doi":"10.1088/1361-6595/ad3e29","DOIUrl":null,"url":null,"abstract":"Time-resolved Langmuir probe diagnostics at the discharge centerline and at three distances from the target ( , , and ) was carried out during long positive voltage pulses (a duration of and a preset positive voltage of ) in bipolar high-power impulse magnetron sputtering of a Ti target (a diameter of ) using an unbalanced magnetron. Fast-camera spectroscopy imaging recorded light emission from Ar and Ti atoms and singly charged ions during positive voltage pulses. It was found that during the long positive voltage pulse, the floating and the plasma potentials suddenly decrease, which is accompanied by the presence of anode light located on the discharge centerline between the target center and the magnetic null of the magnetron’s magnetic field. These light patterns are related to the ignition of a reverse discharge, which leads to the subsequent rise in the plasma and the floating potentials. The reversed discharge is burning up to the end of the positive voltage pulse, but the plasma and floating potentials have lower values than the values from the initial part of the positive voltage pulse. Secondary electron emission induced by the impinging Ar+ ions to the grounded surfaces in the vicinity of the discharge plasma together with the mirror configuration of the magnetron magnetic field are identified as the probable causes of the charge double-layer structure formation in front of the target and the ignition of the reverse discharge.","PeriodicalId":20192,"journal":{"name":"Plasma Sources Science and Technology","volume":"41 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-05-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Sources Science and Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/1361-6595/ad3e29","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Time-resolved Langmuir probe diagnostics at the discharge centerline and at three distances from the target ( , , and ) was carried out during long positive voltage pulses (a duration of and a preset positive voltage of ) in bipolar high-power impulse magnetron sputtering of a Ti target (a diameter of ) using an unbalanced magnetron. Fast-camera spectroscopy imaging recorded light emission from Ar and Ti atoms and singly charged ions during positive voltage pulses. It was found that during the long positive voltage pulse, the floating and the plasma potentials suddenly decrease, which is accompanied by the presence of anode light located on the discharge centerline between the target center and the magnetic null of the magnetron’s magnetic field. These light patterns are related to the ignition of a reverse discharge, which leads to the subsequent rise in the plasma and the floating potentials. The reversed discharge is burning up to the end of the positive voltage pulse, but the plasma and floating potentials have lower values than the values from the initial part of the positive voltage pulse. Secondary electron emission induced by the impinging Ar+ ions to the grounded surfaces in the vicinity of the discharge plasma together with the mirror configuration of the magnetron magnetic field are identified as the probable causes of the charge double-layer structure formation in front of the target and the ignition of the reverse discharge.
在使用非平衡磁控管对 Ti 靶(直径为 )进行双极高功率脉冲磁控管溅射时,在放电中心线和距靶三个距离( 、 、 和 )处进行了时间分辨朗缪尔探针诊断。在正电压脉冲期间,快速相机光谱成像记录了 Ar 和 Ti 原子以及单电荷离子的光发射。研究发现,在长正向电压脉冲期间,浮动电位和等离子体电位突然降低,同时在靶中心和磁控管磁场磁空之间的放电中心线上出现阳极光。这些光斑与反向放电的点燃有关,反向放电导致等离子体和浮动电位随之上升。反向放电一直燃烧到正电压脉冲结束,但等离子体和浮动电位的值低于正电压脉冲初始部分的值。放电等离子体附近接地表面的 Ar+ 离子撞击引起的二次电子发射以及磁控管磁场的镜面配置被认为是靶前电荷双层结构形成和反向放电点燃的可能原因。