Skip to main navigation Skip to search Skip to main content

Overview of the activities on the ITER fast-ion loss detector

  • R. Marques*
  • , L. Sanchis
  • , J. Galdón-Quiroga
  • , Antti Snicker
  • , J. Ayllon-Guerola
  • , N. Azais
  • , O. Brown
  • , F. J. Ferrer
  • , J. Hidalgo-Salaverri
  • , O. J. Hyvärinen
  • , R. Marsh
  • , L. Morgan
  • , K. Patel
  • , D. Peña-Arevalo
  • , A. Reyner-Viñolas
  • , M. Rodriguez-Ramos
  • , J. Rueda-Rueda
  • , P. Shigin
  • , P. Vicente
  • , M. Videla
  • C. Vorpahl, J. Williams, P. Wise, M. Garcia-Munoz, M. Kocan, S. Di Sarra, J. Gonzalez-Martin
*Corresponding author for this work
  • University of Seville
  • Leonardo S.p.A
  • Princeton University
  • United Kingdom Atomic Energy Authority (UKAEA)
  • Tokamak Energy Ltd
  • University of California Irvine (UCI)
  • ITER Organization
  • ICPS

Research output: Contribution to journalArticleScientificpeer-review

Abstract

Latest advancements in the design of the ITER Lost Alpha Monitor diagnostic, also known as fast-ion loss detector (FILD), are detailed in this article. Advanced Hamiltonian full-orbit simulations are performed to estimate the velocity-space of fast-ion fluxes on the diagnostic probe head. Using the ASCOT code, these fluxes are characterized for different spatial spectra of externally applied 3D fields and probe head insertion depths. The probe head is inserted into the scrape-off layer (positioned at the level of the first wall) using a reciprocating system featuring an internal moving shaft, double bellows for vacuum integrity, and an electric actuator with a total radial stroke of (Formula presented) (Formula presented) 50 cm. Detailed structural, electromagnetic, and dynamic analyses of this reciprocating system are presented to validate its mechanical robustness against gravitational and induced electromagnetic forces. Thermomechanical modeling of heat loads on the probe head is used to estimate mechanical stresses and scintillator operating temperature.The light pattern emitted by the scintillator is computed using the FILDSIM code, which incorporates scintillator efficiency and orbit simulations. A 14 m long optical relay, featuring free-form mirrors and radiation-hardened lenses, collects and transmits the scintillator light into a shielding cabinet in the port cell. This cabinet houses the instrumentation for data acquisition (DAQ), digitizers for Faraday Cups, photomultiplier tubes, and charge couple device cameras. Monte Carlo simulations estimate radiation-induced noise on the scintillator and the effectiveness of DAQ shielding in the interspace. Together, these advancements ensure an acceptable signal-to-noise ratio of the Lost Alpha Monitor throughout the entire ITER operation.

Original languageEnglish
Article number075010
JournalPlasma Physics and Controlled Fusion
Volume68
Issue number7
DOIs
Publication statusPublished - 2026
MoE publication typeA1 Journal article-refereed

Funding

This work has been carried out within the framework of the EUROfusion Consortium, funded by the European Union via the Euratom Research and Training Programme (Grant Agreement No 101052200 - EUROfusion).

UN SDGs

This output contributes to the following UN Sustainable Development Goals (SDGs)

  1. SDG 3 - Good Health and Well-being
    SDG 3 Good Health and Well-being
  2. SDG 7 - Affordable and Clean Energy
    SDG 7 Affordable and Clean Energy

Keywords

  • fast-ion loss detector
  • fast-ions
  • FILD
  • ITER
  • lost alpha monitor
  • nuclear fusion
  • plasma diagnostic

Fingerprint

Dive into the research topics of 'Overview of the activities on the ITER fast-ion loss detector'. Together they form a unique fingerprint.

Cite this