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3D Depth Profile Reconstruction of Segregated Impurities Using Secondary Ion Mass Spectrometry
Published on: April 29, 2020
Tomographic imaging system for measuring impurity line emission in a field-reversed configuration
The Review of Scientific Instruments
|November 7, 2012
Summary
A new 16-chord optical tomography system measures argon emission in a field-reversed configuration (FRC) plasma. This system reveals impurity ion diffusion rates crucial for understanding FRC plasma confinement.
Area of Science:
- Plasma Physics
- Optical Diagnostics
- Fusion Energy Research
Background:
- Field-reversed configurations (FRCs) are a promising magnetic confinement fusion approach.
- Accurate measurement of impurity ion transport is essential for optimizing FRC plasma stability and confinement.
- Existing diagnostic methods may have limitations in spatial and temporal resolution for FRC plasmas.
Purpose of the Study:
- To develop and implement a 16-chord optical tomography system for FRC plasmas.
- To measure the 2D emissivity profiles of impurity ions (singly ionized argon).
- To determine the radial, cross-field diffusion coefficients of impurity ions during FRC equilibrium.
Main Methods:
- A 16-chord optical tomography system with two fans of eight chords was implemented.
- Photomultiplier tubes (PMTs) with narrow band-pass filters centered at 434.8 nm measured argon emission.
- Argon gas was introduced via a puff valve during FRC formation.
- Reconstruction algorithms generated time-dependent, 2D emissivity profiles.
Main Results:
- The system achieved a spatial resolution of 1.5 cm.
- Background noise was less than 10% of the argon emission signal.
- Radial, cross-field diffusion coefficients were determined to be in the range of 10–10^3 m²/s during FRC equilibrium.
Conclusions:
- The developed optical tomography system is effective for diagnosing FRC plasmas.
- The measured diffusion coefficients provide critical data for FRC plasma modeling and improvement.
- This diagnostic capability advances the understanding of impurity transport in FRCs.