M. Van Schoor
École Normale Supérieure
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by M. Van Schoor.
Physics of Plasmas | 2014
J. Ongena; A. Messiaen; D. Van Eester; B. Schweer; P. Dumortier; F. Durodié; Yevgen O. Kazakov; F. Louche; M. Vervier; R. Koch; A. Krivska; A. Lyssoivan; M. Van Schoor; T. Wauters; V. Borsuk; O. Neubauer; O. Schmitz; G. Offermans; Y. Altenburg; C. Baylard; D. Birus; S. Bozhenkov; D. Hartmann; J. Kallmeyer; S. Renard; R. C. Wolf; Tünde Fülöp
The current status of the mechanical and electromagnetic design for the ICRF antenna system for W7-X is presented. Two antenna plugins are discussed: one consisting of a pair of straps with pre-matching to cover the first frequency band, 25–38 MHz, and a second one consisting of two short strap triplets to cover a frequency band around 76 MHz. This paper focusses on the two strap antenna for the lower frequency band. Power coupling of the antenna to a reference plasma profile is studied with the help of the codes TOPICA and Microwave Studio that deliver the scattering matrix needed for the optimization of the geometric parameters of the straps and antenna box. Radiation power spectra for different phasings of the two straps are obtained using the code ANTITER II and different heating scenario are discussed. The potential for heating, fast particle generation, and current drive is discussed. The problem of RF coupling through the plasma edge and of edge power deposition is summarized. Important elements of the complete ion cyclotron resonance heating system are discussed: a resonator circuit with tap feed to limit the maximum voltage in the system, and a decoupler to counterbalance the large mutual coupling between the 2 straps. The mechanical design highlights the challenges encountered with this antenna: adaptation to a large variety of plasma configurations, the limited space within the port to accommodate the necessary matching components and the watercooling needed for long pulse operation.
Review of Scientific Instruments | 2013
I. Shesterikov; Y. Xu; M. Berte; P. Dumortier; M. Van Schoor; M. Vergote; B. Schweer; G. Van Oost
Gas puff imaging (GPI) [S. J. Zweben, D. P. Stotler et al., Phys. Plasmas 9, 1981 (2002); R. J. Maqueda, G. A. Wurden et al., Rev. Sci. Instrum. 74, 2020 (2003)] is a powerful diagnostic that permits a two-dimensional measurement of turbulence in the edge region of a fusion plasma and is based on the observation of the local emission of a neutral gas, actively puffed into the periphery of the plasma. The developed in-vessel GPI telescope observes the emission from the puffed gas along local (at the puff) magnetic field lines. The GPI telescope is specially designed to operate in severe TEXTOR conditions and can be treated as a prototype for the GPI systems on next generation machines. Also, the gas puff nozzle is designed to have a lower divergence of the gas flow than previous GPI diagnostics. The resulting images show poloidally and radially propagating structures, which are associated with plasma blobs. We demonstrate that the local gas puff does not disturb plasma properties. Our results indicate also that the neutral gas emission intensity is more sensitive to the electron density than the electron temperature. Here, we present implementation details of the GPI system on TEXTOR and discuss some design and diagnostic issues related to the development of GPI systems in general.
RADIOFREQUENCY POWER IN PLASMAS: Proceedings of the 20th Topical Conference | 2014
J. Ongena; A. Messiaen; P. Dumortier; F. Durodié; Ye. O. Kazakov; F. Louche; B. Schweer; M. Vervier; D. Van Eester; R. Koch; A. Krivska; A. Lyssoivan; M. Van Schoor; T. Wauters; V. Borsuk; O. Neubauer; O. Schmitz; G. Offermans; Y. Altenburg; Ch. Baylard; D. Birus; S. Bozhenkov; D. Hartmann; J. Kallmeyer; S. Renard; R. C. Wolf
The current status of the mechanical and electromagnetic design for the ICRF antenna system for W7-X is presented. Two antenna plugins are discussed: one consisting of a pair of straps with pre-matching to cover the first frequency band 25-38 MHz and a second one consisting of two short strap triplets to cover a frequency band around 76 MHz. This paper focusses on the two strap antenna for the lower frequency band. Power coupling of the antenna to a reference plasma profile is studied with the help of the codes TOPICA and Microwave Studio, that deliver the scattering matrix needed for the optimization of the geometric parameters of the straps and antenna box. Radiation power spectra for different phasings of the two straps are obtained using the code ANTITER II and different heating scenarii are discussed. The potential for heating, fast particle generation and current drive is discussed. The problem of RF coupling through the plasma edge and of edge power deposition is summarized. The system contains a p...
RADIO FREQUENCY POWER IN PLASMAS: Proceedings of the 18th Topical Conference | 2009
T. Wauters; D. Douai; S. Bremond; E. de la Cal; G. Lombard; A. Lyssoivan; Brigitte Pegourie; E. Tsitrone; M. Van Schoor; G. Van Oost
Wall conditioning techniques applicable in the presence of the high toroidal magnetic field will be required for the operation of ITER for tritium removal, isotopic ratio control and recovery to normal operation after disruptions. Recently ion cyclotron wall conditioning (ICWC) experiments have been carried out on Tore Supra in order to assess the efficiency of this technique in ITER relevant conditions. The ICRF discharges were operated in He/H2 mixtures at the Tore Supra nominal field (3.8 T) and a RF frequency of 48 MHz, i.e. within the ITER operational space. RF pulses of 60 s (max.) were applied using a standard Tore Supra two‐strap resonant double loop antenna in ICWC mode, operated either in π or 0‐phasing with a noticeable improvement of the RF coupling in the latter case. In order to assess the efficiency of the technique for the control of isotopic ratio the wall was first preloaded using a D2 glow discharge. After 15 minutes of ICWC in He/H2 gas mixtures the isotopic ratio was altered from 4% t...
RADIO FREQUENCY POWER IN PLASMAS: Proceedings of the 21st Topical Conference | 2015
M. Tripský; T. Wauters; A. Lyssoivan; A. Křivská; F. Louche; M. Van Schoor; J.-M. Noterdaeme
Discharges produced and sustained by ion cyclotron range of frequency (ICRF) waves in absence of plasma current will be used on ITER for (ion cyclotron-) wall conditioning (ICWC). The here presented simulations aim at ensuring that the ITER ICRH&CD system can be safely employed for ICWC and at finding optimal parameters to initiate the plasma.The 1D Monte Carlo code RFdinity1D3V was developed to simulate ICRF discharge initiation. The code traces the electron motion along one toroidal magnetic field line, accelerated by the RF field in front of the ICRF antenna. Electron collisions in the calculations are handled by a Monte Carlo procedure taking into account their energies and the related electron collision cross sections for collisions with H2, H2+ and H+. The code also includes Coulomb collisions between electrons and ions (e − e, e − H2+, e − H+).We study the electron multiplication rate as a function of the RF discharge parameters (i) antenna input power (0.1-5MW), and (ii) the neutral pressure (H2) ...
RADIOFREQUENCY POWER IN PLASMAS: Proceedings of the 20th Topical Conference | 2014
M. Tripsky; T. Wauters; A. Lyssoivan; R. Koch; V. Bobkov; M. Vervier; G. Van Oost; M. Van Schoor; Textor Team
The radio-frequency (RF) plasma production technique in the ion cyclotron range of frequency (ICRF) attracts growing attention among fusion experts because of its high potential for solving several basic problems of reactor-oriented superconducting fusion machines, such as ICRF wall conditioning in tokamaks and stellarators (Teu2009=u20093−5eV, ne<1012cm−3), ICRF-assisted tokamak start-up and target plasma production (neu2009=u20091013cm−3) in stellarators. Plasma initiation by ICRF has been studied intensively using single particle descriptions and basic analytic models. To further improve the present understanding on plasma production employing the vacuum RF field of ICRF antennas in toroidal devices in presence of the toroidal magnetic field, and its parametric dependencies a Monte Carlo code has been developed. The 1D code RFdinity1D describes the motion of electrons, accelerated by the RF field in front of the ICRF antenna, along one toroidal magnetic field line. Dependent on their individual energies and the relate...
Physical Review Letters | 2006
Y. Xu; R.R. Weynants; S. Jachmich; M. Van Schoor; M. Vergote; Peter Peleman; Mw Jakubowski; M. Mitri; D. Reiser; B. Unterberg; Kh Finken
Physical Review Letters | 2013
I. Shesterikov; Y. Xu; G. R. Tynan; P. H. Diamond; S. Jachmich; P. Dumortier; M. Vergote; M. Van Schoor; G. Van Oost
Nature Physics | 2017
Ye. O. Kazakov; J. Ongena; John Wright; S. Wukitch; E. Lerche; M. Mantsinen; D. Van Eester; T. Craciunescu; V. Kiptily; Y. Lin; M. Nocente; F. Nabais; M. F. F. Nave; Y. Baranov; J. Bielecki; R. Bilato; V. Bobkov; Kristel Crombé; A. Czarnecka; J. M. Faustin; R. Felton; M. Fitzgerald; D. Gallart; L. Giacomelli; T. Golfinopoulos; A. Hubbard; P. Jacquet; Thomas Johnson; M. Lennholm; T. Loarer
Contributions To Plasma Physics | 2006
Peter Peleman; S. Jachmich; M. Van Schoor; G. Van Oost; W. Knaepen; C. Boucher