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Neutron emission spectrometer to measure ion temperature on the Fusion Demonstration Plant.
Carle, P J F; Retière, F; Sher, A; Underwood, R; Starosta, K; Hildebrand, M; Barsky, S; Howard, S.
Afiliação
  • Carle PJF; General Fusion Inc., 320-3600 Lysander Lane, Richmond, British Columbia V7B 1C3, Canada.
  • Retière F; TRIUMF, 4004 Wesbrook Mall, Vancouver, British Columbia V6T 2A3, Canada.
  • Sher A; TRIUMF, 4004 Wesbrook Mall, Vancouver, British Columbia V6T 2A3, Canada.
  • Underwood R; TRIUMF, 4004 Wesbrook Mall, Vancouver, British Columbia V6T 2A3, Canada.
  • Starosta K; Department of Chemistry, Simon Fraser University, 8888 University Dr., Burnaby, British Columbia V5A 1S6, Canada.
  • Hildebrand M; General Fusion Inc., 320-3600 Lysander Lane, Richmond, British Columbia V7B 1C3, Canada.
  • Barsky S; General Fusion Inc., 320-3600 Lysander Lane, Richmond, British Columbia V7B 1C3, Canada.
  • Howard S; General Fusion Inc., 320-3600 Lysander Lane, Richmond, British Columbia V7B 1C3, Canada.
Rev Sci Instrum ; 93(11): 113539, 2022 Nov 01.
Article em En | MEDLINE | ID: mdl-36461414
ABSTRACT
General Fusion is building the Fusion Demonstration Plant to demonstrate a magnetized target fusion scheme in which a deuterium plasma is heated from 200 eV to 10 keV by piston-driven compression of a liquid-lithium liner. The multilayer coaxial time-of-flight neutron emission spectrometer is designed to measure the ion temperature near peak compression at which time the neutron yield will approach 1018 neutrons/s. The neutron energy distribution is expected to be Gaussian since the machine uses no neutral beam or radio-frequency heating. In this case, analysis shows that as few as 500 coincidence events should be sufficient to accurately measure the ion temperature. This enables a fast time resolution of 10 µs, which is required to track the rapid change in temperature approaching peak compression. We overcome the challenges of neutron pile-up and event ambiguity with a compact design having two layers of segmented scintillators. The error in the ion temperature measurement is computed as a function of the neutron spectrometer's geometric parameters and used to optimize the design for the case of reaching 10 keV at peak compression.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article