Abstract

Based on the nonlinear three-wave interaction model including driving and dissipation, we construct a system to describe the nonlinear interaction between energetic particle induced geodesic acoustic mode (EGAM) and the drift waves turbulence in the Dimits shift region, and study both analytically and numerically the linear growth and nonlinear oscillation phases of the system, respectively. Further numerical results show that, without the contribution of EGAM, the system goes through limited cycle oscillation to period doubling, and finally route to chaos with the change of the linear drive/dissipation rate. On this basis, the nonlinear saturated “Dimits region” of the system is constructed, which is then used to study the influence of EGAM on the drift wave in the Dimits region. The results show that for EGAM with different amplitude and frequency, the modulated drift wave can be either excited or suppressed, partly reproduces the results from large scale simulation. Finally, We use the method of phase space analysis to give the corresponding explanation.

Highlights

  • The results show that for energetic particle induced geodesic acoustic mode (EGAM) with different amplitude and frequency, the modulated drift wave can be either excited or suppressed, partly reproduces the results from large scale simulation

  • 度, 和 energetic particle induced geodesic acoustic mode (EGAM) 的振荡频率与漂移波-ZFZF 系统演 化到“大极限环”的周期振荡态的时间尺度之比, 解 释了相空间具有不同振荡模式的原因, 并定性地给 出此模型下漂移波被 EGAM 驱动或抑制的条件

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Summary

Introduction

基于包含驱动和阻尼的三波非线性相互作用模型 , 构建了一个描述高能量粒子测地声模 (EGAM) 与 Dimits 区漂移波湍流相互作用的系统, 并在系统的线性增长及非线性振荡阶段分别进行了解析和数值研究. 最 后, 作为本工作最重要的结果, 在模型中引入 EGAM, 来研究 EGAM 与 Dimits 区漂移波的相 互作用. 本文的结构安排如下: 第 2 节引入理论模型; 第 3 节分析了包含源和汇的耦合漂移-ZFZF 系统的非 线性演化; 第 4 节研究了 EGAM 对 Dimits区漂移 波的影响; 第 5 节给出简单的总结和讨论. 其中φ0 , φ1 , φZ 分别代表泵浦波、边带模和 ZFZF 的 振幅, 即 Ωj = φje−iωjt(j = 0, 1, Z); φE 代表 EGAM 的幅度, ωE 代表 EGAM 的频率1; γ0 代表泵浦波 在忽略 EGAM 的影响 ( φE cos(ωEt)) 时, 方程 (1) 描述了漂移波和 ZFZF 的相互作用.

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