A new method to obtain the mean energy of fast electron losses in fusion plasmas using a versatile multi-energy hard x-ray (HXR) detector is presented. The method is based on measuring the thick-target emission of tungsten in the divertor region produced by fast electron losses interacting with the target and modeling the tungsten spectra by a Monte Carlo code which simulates the interaction between a beam of electrons and a solid target. The mean energy of the fast electron losses is determined through the comparison between the experimental and synthetic emission. The results show that fast electron losses during lower hybrid current drive discharges at WEST have a mean energy of 90–140 keV and represent only 2% of the total heat flux at the target. Additionally, anisotropic HXR emission has been detected for the first time at the WEST core and edge plasma, with opposite directions. It is due to the forward-peak emission of two distinctive populations of fast electrons: co-current fast electrons in the core and counter-current fast electron losses at the inner strike point. In view of future experiments like ITER where electron cyclotron current drive will generate a fast electron population, this technique could serve as a real-time monitor of fast electron losses and eventually feed an actuator on the current drive generation.
This paper presents a new method to measure the mean energy of fast electron losses in fusion plasmas using a multi-energy hard X-ray detector. The method models the interaction between fast electrons and a solid target to determine the mean energy. The results show that fast electron losses during lower hybrid current drive on WEST have a mean energy of 90-140 keV and represent only 2% of the total heat flux. The paper also reports the first detection of anisotropic hard X-ray emission in the core and edge plasma, indicating the presence of co-current and counter-current fast electron populations.