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HL-2M托卡马克等离子体高场侧的合成电子回旋辐射分析。

Analysis of synthetic electron cyclotron emission from the high field side of HL-2M tokamak plasmas.

作者信息

Yu X, Shi Z B, Jiang M, Yu G Y, Zhu Y L, Yang Z C, Chen W, Zhu Y R, Fang K R, Tong R H, Han J H, Zhang X R

机构信息

Southwestern Institute of Physics, Chengdu 610041, China.

Department of Electrical and Computer Engineering, University of California, Davis, California 95616, USA.

出版信息

Rev Sci Instrum. 2022 Aug 1;93(8):083518. doi: 10.1063/5.0098907.

Abstract

A synthetic electron cyclotron emission (ECE) diagnostic is used to interpret ECE signals from preset plasma equilibrium profiles, including magnetic field, electron density, and electron temperature. According to the simulation results, the electron temperature (T) profile covering the harmonic overlap region can be obtained by receiving ECE signals at the high field side (HFS) of the HL-2M plasma. The third harmonic ECE at the low field side (LFS) cannot pass through the second harmonic resonance layer at the HFS unless the optical thickness (τ) of the second harmonic becomes gray (τ ≤ 2). In addition, the impact of the relativistic frequency down-shift has been evaluated and corrected. The measurable range of the HFS ECE has been calculated by scanning different parameters (electron density, temperature, and magnetic field). Higher plasma parameters allow a wider radial range of electron temperature measurements. The minimum inner measurable position can reach R = 120 cm (r/a = -0.89) when the product of core temperature (T) and density (n) is greater than 35 × 10 keV m, which is extended by more than 30 cm inward compared with that of the LFS measurement. The HFS ECE will greatly improve the diagnostic ability of ECE systems on the HL-2M tokamak.

摘要

一种合成电子回旋辐射(ECE)诊断方法被用于从预设的等离子体平衡分布(包括磁场、电子密度和电子温度)来解释ECE信号。根据模拟结果,通过在HL-2M等离子体的高场侧(HFS)接收ECE信号,可以获得覆盖谐波重叠区域的电子温度(T)分布。低场侧(LFS)的三次谐波ECE除非二次谐波的光学厚度(τ)变为灰色(τ≤2),否则无法穿过高场侧的二次谐波共振层。此外,已经评估并校正了相对论频率下移的影响。通过扫描不同参数(电子密度、温度和磁场)计算了高场侧ECE的可测量范围。更高的等离子体参数允许更宽的电子温度测量径向范围。当核心温度(T)与密度(n)的乘积大于35×10keV·m时,最小内部可测量位置可达到R = 120cm(r/a = -0.89),与低场侧测量相比向内扩展了30多厘米。高场侧ECE将大大提高ECE系统对HL-2M托卡马克的诊断能力。

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