J. Cazabonne, S. Coda, Joan Decker, O. Krutkin, Umesh Kumar, Yves Savoye-Peysson
{"title":"Impact of microwave beam scattering by density fluctuations on the Electron-Cyclotron power deposition profile in tokamaks","authors":"J. Cazabonne, S. Coda, Joan Decker, O. Krutkin, Umesh Kumar, Yves Savoye-Peysson","doi":"10.1088/1741-4326/ad1af6","DOIUrl":null,"url":null,"abstract":"\n Electron-Cyclotron waves are a tool commonly used in tokamaks, in particular to drive current. Their ability to drive current in a very localized manner renders them an optimal tool for MHD mode mitigation. However, such applications require high accuracy and good control of the power deposition location to efficiently target the magnetic islands. It has been indirectly observed that the suprathermal electron distribution, resulting from the wave absorption, is broader than what is expected from experimentally-constrained forward drift-kinetic modeling. The present paper explores the possibility that beam scattering through the turbulent edge of the plasma may explain this observed discrepancy. In particular, full-wave studies exhibit three beam broadening regimes, from superdiffusive to diffusive, with an intermediate regime characterized by a Lorentzian beam profile with a slightly increased full-width at half maximum with respect to the quiet plasma case. In the Tokamak à Configuration Variable, dedicated plasma scenarios have been developed to test this hypothesis. A realistic worst-case fluctuation scenario falls into this intermediate beam broadening regime. By comparing the experimental hard X-ray emission from suprathermal electron Bremmstrahlung with the emission calculated by coupling a full-wave model to a Fokker-Planck solver, it is shown that that, in the tested cases, the beam broadening is not sufficient to explain the aforementioned discrepancy between simulation and experiment and that another mechanism must play the main role in broadening the suprathermal electron distribution.","PeriodicalId":503481,"journal":{"name":"Nuclear Fusion","volume":"43 4","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-01-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Fusion","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/1741-4326/ad1af6","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
Electron-Cyclotron waves are a tool commonly used in tokamaks, in particular to drive current. Their ability to drive current in a very localized manner renders them an optimal tool for MHD mode mitigation. However, such applications require high accuracy and good control of the power deposition location to efficiently target the magnetic islands. It has been indirectly observed that the suprathermal electron distribution, resulting from the wave absorption, is broader than what is expected from experimentally-constrained forward drift-kinetic modeling. The present paper explores the possibility that beam scattering through the turbulent edge of the plasma may explain this observed discrepancy. In particular, full-wave studies exhibit three beam broadening regimes, from superdiffusive to diffusive, with an intermediate regime characterized by a Lorentzian beam profile with a slightly increased full-width at half maximum with respect to the quiet plasma case. In the Tokamak à Configuration Variable, dedicated plasma scenarios have been developed to test this hypothesis. A realistic worst-case fluctuation scenario falls into this intermediate beam broadening regime. By comparing the experimental hard X-ray emission from suprathermal electron Bremmstrahlung with the emission calculated by coupling a full-wave model to a Fokker-Planck solver, it is shown that that, in the tested cases, the beam broadening is not sufficient to explain the aforementioned discrepancy between simulation and experiment and that another mechanism must play the main role in broadening the suprathermal electron distribution.
电子-回旋加速器波是托卡马克中常用的一种工具,特别是用于驱动电流。电子-环电子波能够以非常局部的方式驱动电流,因此是减缓 MHD 模式的最佳工具。然而,这种应用需要高精度和良好的功率沉积位置控制,以便有效地瞄准磁岛。据间接观察,波吸收产生的过热电子分布比实验约束的前向漂移动力学建模所预期的要宽。本文探讨了通过等离子体湍流边缘的光束散射可能解释这种观察到的差异的可能性。特别是,全波研究显示了从超扩散到扩散的三种光束展宽机制,中间机制的特征是洛伦兹光束轮廓,与静态等离子体情况相比,半最大全宽略有增加。在托卡马克 à 配置变量中,开发了专门的等离子体方案来测试这一假设。现实中最糟糕的波动情况就属于这种中间光束展宽机制。通过比较实验中超热电子布赖姆斯特拉发射的硬 X 射线辐射和全波模型与福克-普朗克求解器耦合计算的辐射,结果表明,在测试的情况下,光束增宽不足以解释上述模拟与实验之间的差异,另一种机制必须在增宽超热电子分布方面发挥主要作用。