{"title":"用于沉积过程的中压电容耦合等离子体的高级Pic-Mcc模拟","authors":"Jin Seok Kim, H. Lee, H. J. Kim","doi":"10.1109/PLASMA.2017.8496109","DOIUrl":null,"url":null,"abstract":"A particle-in-cell (PIC) simulation has been usually utilized for observing plasma kinetics in low pressure [1]because of long simulation time as PIC uses a huge amount of computational particles to treat collisions with neutral gas using Monte Carlo collision (MCC) method. In order to simulate high or intermediate pressure discharges, there are three limitations which slow down the total computation time: (1) many simulation particles are needed as plasma density increases. (2) a very short time step is required in MCC process. (3) many collisional reactions should be included. To overcome these limitations, we approach in three ways: (1) parallelization of PIC simulation with Graphics Processing Units (GPUs), (2) improvement of MCC method, (3) and combination with a fluid model for heavy particle collisions. In this presentation, ion transport phenomena are investigated at the wafer edge in a capacitively coupled plasma (CCP) reactor under an intermediate pressure of a few Torr. The effects of waferfocus ring gap, focus ring height, and the dielectric constant are investigated on the neutral and the ion fluxes and the ion energy and angle distribution (IAEDF), and compared with the preceded results [2–3]for the effect of the wafer-focus ring property.","PeriodicalId":145705,"journal":{"name":"2017 IEEE International Conference on Plasma Science (ICOPS)","volume":"81 1-2 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2017-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Advanced Pic-Mcc Simulation for an Intermediate-Pressure Capacitively Coupled Plasma for Deposition Process\",\"authors\":\"Jin Seok Kim, H. Lee, H. J. Kim\",\"doi\":\"10.1109/PLASMA.2017.8496109\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A particle-in-cell (PIC) simulation has been usually utilized for observing plasma kinetics in low pressure [1]because of long simulation time as PIC uses a huge amount of computational particles to treat collisions with neutral gas using Monte Carlo collision (MCC) method. In order to simulate high or intermediate pressure discharges, there are three limitations which slow down the total computation time: (1) many simulation particles are needed as plasma density increases. (2) a very short time step is required in MCC process. (3) many collisional reactions should be included. To overcome these limitations, we approach in three ways: (1) parallelization of PIC simulation with Graphics Processing Units (GPUs), (2) improvement of MCC method, (3) and combination with a fluid model for heavy particle collisions. In this presentation, ion transport phenomena are investigated at the wafer edge in a capacitively coupled plasma (CCP) reactor under an intermediate pressure of a few Torr. The effects of waferfocus ring gap, focus ring height, and the dielectric constant are investigated on the neutral and the ion fluxes and the ion energy and angle distribution (IAEDF), and compared with the preceded results [2–3]for the effect of the wafer-focus ring property.\",\"PeriodicalId\":145705,\"journal\":{\"name\":\"2017 IEEE International Conference on Plasma Science (ICOPS)\",\"volume\":\"81 1-2 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2017-05-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2017 IEEE International Conference on Plasma Science (ICOPS)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PLASMA.2017.8496109\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2017 IEEE International Conference on Plasma Science (ICOPS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PLASMA.2017.8496109","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
由于采用蒙特卡罗碰撞(Monte Carlo collision, MCC)方法处理与中性气体的碰撞,通常采用粒子池(particle-in-cell, PIC)模拟来观察低压条件下等离子体动力学[1],因为PIC使用了大量的计算粒子,模拟时间长。为了模拟高压或中压放电,有三个限制减慢了总计算时间:(1)随着等离子体密度的增加,需要许多模拟粒子。(2) MCC过程所需的时间步长很短。(3)应包括许多碰撞反应。为了克服这些限制,我们从三个方面着手:(1)图形处理单元(gpu)并行化PIC仿真;(2)改进MCC方法;(3)结合重粒子碰撞流体模型。本文研究了电容耦合等离子体反应器在几托中压下的离子输运现象。研究了聚焦环间隙、聚焦环高度和介电常数对中性离子通量和离子能量角分布(IAEDF)的影响,并与前人的研究结果[2-3]进行了比较。
Advanced Pic-Mcc Simulation for an Intermediate-Pressure Capacitively Coupled Plasma for Deposition Process
A particle-in-cell (PIC) simulation has been usually utilized for observing plasma kinetics in low pressure [1]because of long simulation time as PIC uses a huge amount of computational particles to treat collisions with neutral gas using Monte Carlo collision (MCC) method. In order to simulate high or intermediate pressure discharges, there are three limitations which slow down the total computation time: (1) many simulation particles are needed as plasma density increases. (2) a very short time step is required in MCC process. (3) many collisional reactions should be included. To overcome these limitations, we approach in three ways: (1) parallelization of PIC simulation with Graphics Processing Units (GPUs), (2) improvement of MCC method, (3) and combination with a fluid model for heavy particle collisions. In this presentation, ion transport phenomena are investigated at the wafer edge in a capacitively coupled plasma (CCP) reactor under an intermediate pressure of a few Torr. The effects of waferfocus ring gap, focus ring height, and the dielectric constant are investigated on the neutral and the ion fluxes and the ion energy and angle distribution (IAEDF), and compared with the preceded results [2–3]for the effect of the wafer-focus ring property.