Related Experiment Video
Updated: Jan 3, 2026

06:28
Visualization of Low-Level Gamma Radiation Sources Using a Low-Cost, High-Sensitivity, Omnidirectional Compton Camera
Published on: January 30, 2020
13.1K
Radiometry for the vertical electron cyclotron emission from the runaway electrons at the COMPASS tokamak
The Review of Scientific Instruments
|November 30, 2019
Summary
A new diagnostic system measures nonthermal electron cyclotron emission from runaway electrons in tokamak plasma. This vertical ECE system provides crucial data on runaway electron populations and their generation.
Area of Science:
- Plasma Physics
- Fusion Energy Research
- Diagnostic Techniques
Background:
- Runaway electron (RE) phenomena are of increasing interest in tokamak research.
- Accurate diagnostics are needed to understand RE populations in plasma.
- Nonthermal electron cyclotron emission (ECE) offers a potential diagnostic method.
Purpose of the Study:
- To design and implement a novel diagnostic system for runaway electrons.
- To utilize a heterodyne radiometer for measuring nonthermal ECE.
- To assess the feasibility of diagnosing REs up to 1 MeV.
Main Methods:
- Installation of a vertical ECE (V-ECE) system at the COMPASS tokamak.
- Utilizing a 16-channel heterodyne radiometer with an E2-band horn antenna (76.5-90 GHz).
- Employing the SPECE code for ray-tracing simulations to determine measurement feasibility.
Main Results:
- The V-ECE system is feasible for measuring runaway electrons up to 1 MeV.
- Reflected waves from the tokamak wall were detected due to low plasma optical depth.
- Initial results demonstrate a strong correlation with other RE diagnostics at COMPASS.
Conclusions:
- The V-ECE system is a viable diagnostic tool for runaway electron research.
- The system can provide valuable insights into RE population dynamics and generation mechanisms.
- This diagnostic contributes to advancing the understanding of RE phenomena in tokamaks.
Related Concept Videos
Generating Electromagnetic Radiations
6.5K
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in...
6.5K
Thomson's e/m Experiment
6.3K
In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The magnetic...
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The magnetic...
6.3K
Electromagnetic Fields
2.6K
Electric fields generated by static charges, often referred to as electrostatic fields, are characteristically different from electric fields created by time-varying magnetic fields. While the former is a conservative field, implying that no net work is done on a test charge if it goes around in a complete loop in the field, the latter is, by definition, not a conservative field; net work is done, and it is proportional to the rate of change of magnetic flux.
However, the observation of...
However, the observation of...
2.6K
Atomic Emission Spectroscopy: Overview
3.4K
Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...
3.4K
Atomic Absorption Spectroscopy: Radiation and Light Sources
1.0K
Atomic absorption spectroscopy (AAS) relies on the Beer-Lambert law, which requires that the radiation source emits a narrow range of wavelengths to match the absorption characteristics of the analyte atom. The primary criteria for choosing an appropriate radiation source in AAS is to provide a precise and intense emission at specific wavelengths that will allow accurate detection of the analyte.
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
1.0K
Atomic Emission Spectroscopy: Instrumentation
1.1K
The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers. Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
1.1K

