Dal Molin A, Marcer G, Nocente M, Rebai M, Rigamonti D, Angelone M, Bracco A, Camera F, Cazzaniga C, Craciunescu T, Croci G, Dalla Rosa M, Giacomelli L, Gorini G, Kazakov Y, Khilkevitch E M, Muraro A, Panontin E, Perelli Cippo E, Pillon M, Putignano O, Scionti J, Shevelev A E, Žohar A, Tardocchi M
<a href="https://ror.org/047rmsn51">Institute for Plasma Science and Technology</a>, Consiglio Nazionale delle Ricerche, Milan, Italy.
Department of Physics, <a href="https://ror.org/01ynf4891">University of Milano-Bicocca</a>, Milan, Italy.
Phys Rev Lett. 2024 Aug 2;133(5):055102. doi: 10.1103/PhysRevLett.133.055102.
At present, magnetic confinement fusion devices rely solely on absolute neutron counting as a direct way of measuring fusion power. Absolute counting of deuterium-tritium gamma rays could provide the secondary neutron-independent technique required for the validation of scientific results and as a licensing tool for future power plants. However, this approach necessitates an accurate determination of the gamma-ray-to-neutron branching ratio. The gamma-ray-to-neutron branching ratio for the deuterium-tritium reaction ^{3}H(^{2}H,γ)^{5}He/^{3}H(^{2}H,n)^{4}He was determined in magnetic confinement fusion plasmas at the Joint European Torus in predominantly deuterium beam heated plasmas. The branching ratio was found to be equal to (2.4±0.5)×10^{-5} over the deuterium energy range of (80±20) keV. This accurate determination of the deuterium-tritium branching ratio paves the way for a direct and neutron-independent measurement of fusion power in magnetic confinement fusion reactors, based on the absolute counting of deuterium-tritium gamma rays.
目前,磁约束聚变装置完全依靠绝对中子计数作为测量聚变功率的直接方法。氘 - 氚伽马射线的绝对计数可以提供验证科学结果所需的与中子无关的辅助技术,并作为未来发电厂的许可工具。然而,这种方法需要精确测定伽马射线与中子的分支比。在欧洲联合环面的磁约束聚变等离子体中,在以氘束为主加热的等离子体中测定了氘 - 氚反应(^{3}H(^{2}H,γ)^{5}He/^{3}H(^{2}H,n)^{4}He)的伽马射线与中子的分支比。发现在((80±20))keV的氘能量范围内,分支比等于((2.4±0.5)×10^{-5})。氘 - 氚分支比的这种精确测定为基于氘 - 氚伽马射线绝对计数的磁约束聚变反应堆中聚变功率的直接且与中子无关的测量铺平了道路。