{"title":"Plasma dynamics of individual HiPIMS pulses: imaging study using high-frame-rate camera","authors":"Matjaž Panjan","doi":"10.1088/1361-6595/ad4416","DOIUrl":null,"url":null,"abstract":"A high-frame-rate camera with microsecond-level time resolution was used to make systematic investigations of plasma self-organization and spoke dynamics during individual HiPIMS pulses. The plasma was imaged for a range of argon pressures (0.25–2 Pa) and peak discharge currents (10–400 A) using an Al target. The experiments revealed that plasma evolves through three characteristic stages as the discharge current increases. In stage I, which is present from the current onset and up to ∼25 A, spokes are azimuthally long and rotate in the −Ez× B direction. The spoke behavior is similar to the one observed in DCMS discharges. The number of spokes depends on pressure and the current growth rate. At the lowest pressure (0.25 Pa) a single spoke is present in discharge, while at higher pressures (1–2 Pa) two spokes are most often observed. The spoke velocity depends on the number of spokes, current growth rate and pressure. A single spoke rotates with velocities in the 4–15 km s−1 range, while two spokes rotate in the 1–9 km s−1 range depending on the pressure and growth rate. Following stage I, the plasma undergoes a complex reorganization that is characterized by aperiodic spoke patterns and irregular dynamics. In stage II spokes are less localized, they merge, split and propagate either in the retrograde or prograde direction. After chaotic plasma reorganization, more ordered spoke patterns begin to form. Spokes in stage III are azimuthally shorter, typically exhibit a triangular shape and rotate in the Ez× B direction. In general, the spoke dynamics is less complicated and is only influenced by the pressure. Spokes rotate faster at higher pressures than at lower ones; velocities range from 9 km s−1 at 0.25 Pa to 6 km s−1 at 2 Pa. The spoke velocity in stage III is largely unaffected by the discharge current or number of spokes. Stage III can be further divided into sub-stages, which are characterized by different current growth rates, spoke sizes and shapes. In general, the spoke evolution is highly reproducible for pulses with similar discharge current waveforms.","PeriodicalId":20192,"journal":{"name":"Plasma Sources Science and Technology","volume":"94 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-05-21","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/ad4416","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
A high-frame-rate camera with microsecond-level time resolution was used to make systematic investigations of plasma self-organization and spoke dynamics during individual HiPIMS pulses. The plasma was imaged for a range of argon pressures (0.25–2 Pa) and peak discharge currents (10–400 A) using an Al target. The experiments revealed that plasma evolves through three characteristic stages as the discharge current increases. In stage I, which is present from the current onset and up to ∼25 A, spokes are azimuthally long and rotate in the −Ez× B direction. The spoke behavior is similar to the one observed in DCMS discharges. The number of spokes depends on pressure and the current growth rate. At the lowest pressure (0.25 Pa) a single spoke is present in discharge, while at higher pressures (1–2 Pa) two spokes are most often observed. The spoke velocity depends on the number of spokes, current growth rate and pressure. A single spoke rotates with velocities in the 4–15 km s−1 range, while two spokes rotate in the 1–9 km s−1 range depending on the pressure and growth rate. Following stage I, the plasma undergoes a complex reorganization that is characterized by aperiodic spoke patterns and irregular dynamics. In stage II spokes are less localized, they merge, split and propagate either in the retrograde or prograde direction. After chaotic plasma reorganization, more ordered spoke patterns begin to form. Spokes in stage III are azimuthally shorter, typically exhibit a triangular shape and rotate in the Ez× B direction. In general, the spoke dynamics is less complicated and is only influenced by the pressure. Spokes rotate faster at higher pressures than at lower ones; velocities range from 9 km s−1 at 0.25 Pa to 6 km s−1 at 2 Pa. The spoke velocity in stage III is largely unaffected by the discharge current or number of spokes. Stage III can be further divided into sub-stages, which are characterized by different current growth rates, spoke sizes and shapes. In general, the spoke evolution is highly reproducible for pulses with similar discharge current waveforms.
利用具有微秒级时间分辨率的高帧频照相机对单个 HiPIMS 脉冲期间的等离子体自组织和辐条动力学进行了系统研究。使用一个铝靶,在一系列氩气压力(0.25-2 Pa)和峰值放电电流(10-400 A)条件下对等离子体进行了成像。实验表明,随着放电电流的增加,等离子体会经历三个特征阶段。在第一阶段,即从电流开始到 ∼25 A 时,辐条呈方位长条状,并沿 -Ez× B 方向旋转。辐条行为类似于在 DCMS 放电中观察到的行为。辐条的数量取决于压力和电流增长率。在最低压力(0.25 Pa)下,放电中只出现一根辐条,而在较高压力(1-2 Pa)下,最常见的是两根辐条。辐条速度取决于辐条数量、电流增长率和压力。单根辐条的旋转速度在 4-15 千米/秒之间,而两根辐条的旋转速度在 1-9 千米/秒之间,具体取决于压力和增长速度。在第一阶段之后,等离子体经历了复杂的重组,其特点是非周期性的辐条模式和不规则的动力学。在第二阶段,辐条的局部性较弱,它们合并、分裂并向逆行或顺行方向传播。在混乱的等离子体重组之后,开始形成更有序的辐条模式。第三阶段的辐条方位较短,通常呈三角形,并沿 Ez× B 方向旋转。一般来说,辐条的动力学没有那么复杂,只受压力的影响。压力较高时,辐条的旋转速度比压力较低时要快;速度范围从 0.25 Pa 时的 9 km s-1 到 2 Pa 时的 6 km s-1。阶段 III 还可进一步划分为几个子阶段,其特点是电流增长率、辐条尺寸和形状各不相同。一般来说,对于具有类似放电电流波形的脉冲,辐条的演变具有很高的重现性。