Zhicheng Jiao, D. Dai, rui Ming Zhu, Tao Shao, Buang Wang
{"title":"从第一原理模型看κ-Al2O3 表面充电中离子诱导二次电子发射的非线性变化","authors":"Zhicheng Jiao, D. Dai, rui Ming Zhu, Tao Shao, Buang Wang","doi":"10.1088/2058-6272/ad386b","DOIUrl":null,"url":null,"abstract":"\n Secondary electron emission (SEE) induced by the positive ion is an essential physical process to influence the dynamics of gas discharge which relies on the specific surface material. Surface charging has a significant impact on the material properties, thereby affecting the SEE in the plasma-surface interactions. However, it does not attract enough attention in the previous studies. In this paper, SEE dependent on the charged surface of specific materials is described with the computational method combining a density functional theory (DFT) model from the first-principle theory and the theory of Auger neutralization. The effect of κ-Al2O3 surface charge, as an example, on the ion-induced secondary electron emission coefficient (SEEC) is investigated by analysing the defect energy level and band structure on the charged surface. Simulation results indicate that, with the surface charge from negative to positive, the SEEC of a part of low ionization energy ions (such as Ei = 12.6 eV) increases first and then decreases, exhibiting a nonlinear changing trend. This is quite different from the monotonic decreasing tendency observed in the previous model which simplifies the electronic structure. This irregular increase of the SEEC can be attributed to the lower escaped probability of orbital energy. The results further illustrate that the excessive charge could cause the bottom of the conduction band close to the valence band, thus leading to the decrease of the orbital energy occupied by the excited electrons. The nonlinear change of SEEC demonstrates a more realistic situation of how the electronic structure of material surface influences the SEE process. This work provides an accurate method of calculating SEEC from specific materials, which is urgent in widespread physical scenarios sensitive to surface materials, such as increasingly growing practical applications concerning plasma-surface interactions.","PeriodicalId":506986,"journal":{"name":"Plasma Science and Technology","volume":"10 9","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-03-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Nonlinear change of ion-induced secondary electron emission in the κ-Al2O3 surface charging from first-principle modelling\",\"authors\":\"Zhicheng Jiao, D. Dai, rui Ming Zhu, Tao Shao, Buang Wang\",\"doi\":\"10.1088/2058-6272/ad386b\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"\\n Secondary electron emission (SEE) induced by the positive ion is an essential physical process to influence the dynamics of gas discharge which relies on the specific surface material. Surface charging has a significant impact on the material properties, thereby affecting the SEE in the plasma-surface interactions. However, it does not attract enough attention in the previous studies. In this paper, SEE dependent on the charged surface of specific materials is described with the computational method combining a density functional theory (DFT) model from the first-principle theory and the theory of Auger neutralization. The effect of κ-Al2O3 surface charge, as an example, on the ion-induced secondary electron emission coefficient (SEEC) is investigated by analysing the defect energy level and band structure on the charged surface. Simulation results indicate that, with the surface charge from negative to positive, the SEEC of a part of low ionization energy ions (such as Ei = 12.6 eV) increases first and then decreases, exhibiting a nonlinear changing trend. This is quite different from the monotonic decreasing tendency observed in the previous model which simplifies the electronic structure. This irregular increase of the SEEC can be attributed to the lower escaped probability of orbital energy. The results further illustrate that the excessive charge could cause the bottom of the conduction band close to the valence band, thus leading to the decrease of the orbital energy occupied by the excited electrons. The nonlinear change of SEEC demonstrates a more realistic situation of how the electronic structure of material surface influences the SEE process. This work provides an accurate method of calculating SEEC from specific materials, which is urgent in widespread physical scenarios sensitive to surface materials, such as increasingly growing practical applications concerning plasma-surface interactions.\",\"PeriodicalId\":506986,\"journal\":{\"name\":\"Plasma Science and Technology\",\"volume\":\"10 9\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-03-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Plasma Science and Technology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/2058-6272/ad386b\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Science and Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/2058-6272/ad386b","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
正离子诱导的二次电子发射(SEE)是影响气体放电动力学的一个重要物理过程,它依赖于特定的表面材料。表面充电对材料特性有重大影响,从而影响等离子体与表面相互作用中的 SEE。然而,在以往的研究中,这一问题并没有引起足够的重视。本文结合第一原理理论中的密度泛函理论(DFT)模型和欧杰中和理论,通过计算方法描述了特定材料带电表面对 SEE 的影响。以κ-Al2O3 表面电荷为例,通过分析带电表面的缺陷能级和能带结构,研究了离子诱导的二次电子发射系数(SEEC)的影响。模拟结果表明,随着表面电荷由负转正,部分低电离能离子(如 Ei = 12.6 eV)的二次电子发射系数先增大后减小,呈现非线性变化趋势。这与之前简化电子结构的模型中观察到的单调递减趋势截然不同。SEEC 的这种不规则增加可归因于轨道能量的逸散概率较低。结果进一步说明,过多的电荷可能导致导带底部接近价带,从而导致受激电子占据的轨道能量减少。SEEC 的非线性变化展示了材料表面电子结构如何影响 SEE 过程的更真实情况。这项工作提供了一种计算特定材料 SEEC 的精确方法,这在对表面材料敏感的广泛物理场景中非常迫切,例如日益增多的有关等离子体与表面相互作用的实际应用。
Nonlinear change of ion-induced secondary electron emission in the κ-Al2O3 surface charging from first-principle modelling
Secondary electron emission (SEE) induced by the positive ion is an essential physical process to influence the dynamics of gas discharge which relies on the specific surface material. Surface charging has a significant impact on the material properties, thereby affecting the SEE in the plasma-surface interactions. However, it does not attract enough attention in the previous studies. In this paper, SEE dependent on the charged surface of specific materials is described with the computational method combining a density functional theory (DFT) model from the first-principle theory and the theory of Auger neutralization. The effect of κ-Al2O3 surface charge, as an example, on the ion-induced secondary electron emission coefficient (SEEC) is investigated by analysing the defect energy level and band structure on the charged surface. Simulation results indicate that, with the surface charge from negative to positive, the SEEC of a part of low ionization energy ions (such as Ei = 12.6 eV) increases first and then decreases, exhibiting a nonlinear changing trend. This is quite different from the monotonic decreasing tendency observed in the previous model which simplifies the electronic structure. This irregular increase of the SEEC can be attributed to the lower escaped probability of orbital energy. The results further illustrate that the excessive charge could cause the bottom of the conduction band close to the valence band, thus leading to the decrease of the orbital energy occupied by the excited electrons. The nonlinear change of SEEC demonstrates a more realistic situation of how the electronic structure of material surface influences the SEE process. This work provides an accurate method of calculating SEEC from specific materials, which is urgent in widespread physical scenarios sensitive to surface materials, such as increasingly growing practical applications concerning plasma-surface interactions.