Interpreting observations of ion cyclotron emission from large helical device plasmas with beam-injected ion populations
Creators
- 1. Centre for Fusion, Space and Astrophysics, Department of Physics, Warwick University, Coventry CV4 7AL, United Kingdom of Great Britain and Northern Ireland (United Kingdom)
- 2. National Institute for Fusion Science, National Institutes of Natural Sciences, Toki, Gifu 509-5292 (Japan)
- 3. CCFE, Culham Science Centre, Abingdon, Oxfordshire OX14 3DB, United Kingdom of Great Britain and Northern Ireland (United Kingdom)
- 4. Research Institute for Applied Mechanics, Kyushu University, Kasuga 816-8580 (Japan)
- 5. Department of Physics, Pohang University of Science and Technology, Pohang, Gyeongbuk 37673 (Korea, Republic of)
Description
Ion cyclotron emission (ICE) is detected from all large toroidal magnetically confined fusion (MCF) plasmas. It is a form of spontaneous suprathermal radiation, whose spectral peak frequencies correspond to sequential cyclotron harmonics of energetic ion species, evaluated at the emission location. In ICE phenomenology, an important parameter is the value of the ratio of energetic ion velocity to the local Alfvén speed . Here we focus on ICE measurements from heliotron-stellarator hydrogen plasmas, heated by energetic proton neutral beam injection (NBI) in the large helical device, for which takes values both larger (super-Alfvénic) and smaller (sub-Alfvénic) than unity. The collective relaxation of the NBI proton population, together with the thermal plasma, is studied using a particle-in-cell (PIC) code. This evolves the Maxwell–Lorentz system of equations for hundreds of millions of kinetic gyro-orbit-resolved ions and fluid electrons, self-consistently with the electric and magnetic fields. For LHD-relevant parameter sets, the spatiotemporal Fourier transforms of the fields yield, in the nonlinear saturated regime, good computational proxies for the observed ICE spectra in both the super-Alfvénic and sub-Alfvénic regimes for NBI protons. At early times in the PIC treatment, the computed growth rates correspond to analytical linear growth rates of the magnetoacoustic cyclotron instability (MCI), which was previously identified to underlie ICE from tokamak plasmas. The spatially localised PIC treatment does not include toroidal magnetic field geometry, nor background gradients in plasma parameters. Its success in simulating ICE spectra from both tokamak and, here, heliotron-stellarator plasmas suggests that the plasma parameters and ion energetic distribution at the emission location largely determine the ICE phenomenology. This is important for the future exploitation of ICE as a diagnostic for energetic ion populations in MCF plasmas. The capability to span the super-Alfvénic and sub-Alfvénic energetic ion regimes is a generic challenge in interpreting MCF plasma physics, and it is encouraging that this first principles computational treatment of ICE has now achieved this. (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/1741-4326/ab2ca2Additional details
Identifiers
Publishing Information
- Journal Title
- Nuclear Fusion
- Journal Volume
- 59
- Journal Issue
- 9
- Journal Page Range
- [16 p.]
- ISSN
- 0029-5515
- CODEN
- NUFUAU
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 51093875
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Descriptors DEI
- CYCLOTRON HARMONICS; CYCLOTRON INSTABILITY; FOURIER TRANSFORMATION; ICE; ION EMISSION; LHD DEVICE; MAGNETIC FIELDS; NONLINEAR PROBLEMS; PLASMA BEAM INJECTION; POPULATIONS; PROTONS; SPECTRA; TAIL IONS; TOKAMAK DEVICES
- Descriptors DEC
- BARYONS; BEAM INJECTION; CHARGED PARTICLES; CLOSED PLASMA DEVICES; ELEMENTARY PARTICLES; EMISSION; FERMIONS; HADRONS; HARMONICS; INSTABILITY; INTEGRAL TRANSFORMATIONS; IONS; NUCLEONS; OSCILLATIONS; PLASMA INSTABILITY; PLASMA MICROINSTABILITIES; THERMONUCLEAR DEVICES; TRANSFORMATIONS